a Code for the Combination of Indirect and Direct Constraints on High Energy Physics Models Logo
NPSMEFTd6 Class Reference

A model class for new physics in the form of the dimension-six effective Lagrangian. More...

#include <NPSMEFTd6.h>

+ Inheritance diagram for NPSMEFTd6:

Detailed Description

A model class for new physics in the form of the dimension-six effective Lagrangian.

Author
HEPfit Collaboration

This is a Model class containing parameters and functions associated with the general dimension-six effective Lagrangian. (Use the model name "NPSMEFTd6_LFU_QFU" to assume lepton and quark flavour universality)

In this class we consider the dimension-six effective Lagrangian

\[ \mathcal{L}_\mathrm{eff} = \mathcal{L}_\mathrm{SM} + \sum_i \frac{C_i}{\Lambda^2} \mathcal{O}_i. \]

The implementation is written in the basis of [131]. For convenience, the parameterization also includes operators appearing in other common bases. In particular, the complete set of parameters contains 4 redundancies, given by the coefficients \(C_{2B,2W,DHB,DHW,DB,DW} \), which correspond to operators not included in the basis of [131]. For meaningful physical results one must make sure to include only a complete set of interactions in a given analysis.

Initialization

After creating an instance of the current class with the constructor NPSMEFTd6(), it is required to call the initialization method InitializeModel(). In the Monte Carlo run, the constructor as well as the initialization method are called in InputParser::ReadParameters().

Model parameters

The model parameters of NPSMEFTd6 are summarized below:

Label LaTeX symbol Description
CG \(C_{G} \) The coefficient of the operator \({\cal O}_{G}=f_{ABC}G_{\mu}^{A\nu} G_{\nu}^{B\rho}W_{\rho}^{C\mu}\).
CW \(C_{W} \) The coefficient of the operator \({\cal O}_{W}=\varepsilon_{abc}W_{\mu}^{a\nu} W_{\nu}^{b\rho}W_{\rho}^{b\mu}\).
C2B \(C_{2B} \) The coefficient of the operator \({\cal O}_{2B}=\frac 12 (\partial_\rho B_{\mu\nu})^2\). (Implemented via EOM.)
C2W \(C_{2W} \) The coefficient of the operator \({\cal O}_{2W}=\frac 12 (D_\rho W_{\mu\nu}^{a})^2\). (Implemented via EOM.)
C2BS \(C_{2B}^{SILH} \) The coefficient of the SILH operator \({\cal O}_{2B}^{SILH}=\frac 12 (\partial^\mu B_{\mu\nu})(\partial_\rho B^{\rho\nu})\). (Implemented via EOM.)
C2WS \(C_{2W}^{SILH} \) The coefficient of the operator \({\cal O}_{2W}^{SILH}=\frac 12 (D_\mu W^{a~\!\mu\nu})(D^\rho W_{\rho\nu}^{a})\). (Implemented via EOM.)
CHG \(C_{HG} \) The coefficient of the operator \({\cal O}_{HG}=\big(H^\dagger H\big)G_{\mu\nu}^A G^{A\mu\nu}\).
CHW \(C_{HW} \) The coefficient of the operator \({\cal O}_{HW}=\big(H^\dagger H\big)W_{\mu\nu}^a W^{a\mu\nu}\).
CHB \(C_{HB} \) The coefficient of the operator \({\cal O}_{HB}=\big(H^\dagger H\big)B_{\mu\nu} B^{\mu\nu}\).
CDHB \(C_{DHB} \) The coefficient of the operator \({\cal O}_{DHB}=i\big(D^\mu H^\dagger D^\nu H\big) B_{\mu\nu}\).
CDHW \(C_{DHW}\) The coefficient of the operator \({\cal O}_{DHW}=i\big(D^\mu H^\dagger \sigma^a D^\nu H\big) W_{\mu\nu}^a\).
CDB \(C_{DB} \) The coefficient of the operator \({\cal O}_{DB}=\frac{i}{2}\big(H^\dagger \overset{\leftrightarrow}{D}^\mu H\big) \partial^\nu B_{\mu\nu}\). (Implemented via EOM.)
CDW \(C_{DW}\) The coefficient of the operator \({\cal O}_{DW}=\frac{i}{2}\big(H^\dagger \overset{\leftrightarrow}{D}^{a~\!\mu} H\big) D^\nu W_{\mu\nu}^a\). (Implemented via EOM.)
CWB \(C_{WB} \) The coefficient of the operator \({\cal O}_{HWB}=\big(H^\dagger\sigma^a H\big)W_{\mu\nu}^a B^{\mu\nu}\).
CHD \(C_{HD}\) The coefficient of the operator \({\cal O}_{HD}=\big|H^\dagger D_\mu H\big|^2\).
CT \(C_{T}\) The coefficient of the operator \({\cal O}_{T}=\frac{1}{2} \big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big)^2\).
CHbox \(C_{H\Box}\) The coefficient of the operator \({\cal O}_{H\Box}=\big(H^\dagger H\big)\Box\big(H^\dagger H\big)\).
CH \(C_{H}\) The coefficient of the operator \({\cal O}_{H}=\big(H^\dagger H\big)^3\).
CHL1_kk, CHL1_klr, CHL1_kli \( (C_{HL}^{(1)})_{kk}, \mbox{Re}\big[(C_{HL}^{(1)})_{kl}\big], \mbox{Im}\big[(C_{HL}^{(1)})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HL}^{(1)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{L^i}\,\gamma^\mu L^j\big)\), for \(i,j=1,2,3\).
CHL3_kk, CHL3_klr, CHL3_kli \( (C_{HL}^{(3)})_{kk}, \mbox{Re}\big[(C_{HL}^{(3)})_{kl}\big], \mbox{Im}\big[(C_{HL}^{(3)})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HL}^{(3)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{L^i}\,\gamma^\mu \sigma^a L^j\big)\), for \(i,j=1,2,3\).
CHe_kk, CHe_klr, CHe_kli \( (C_{He})_{kk}, \mbox{Re}\big[(C_{He})_{kl}\big], \mbox{Im}\big[(C_{He})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{He})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{E^i}\,\gamma^\mu E^j\big)\), for \(i,j=1,2,3\).
CHQ1_kk, CHQ1_klr, CHQ1_kli \( (C_{HQ}^{(1)})_{kk}, \mbox{Re}\big[(C_{HQ}^{(1)})_{kl}\big], \mbox{Im}\big[(C_{HQ}^{(1)})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HQ}^{(1)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{Q^i}\,\gamma^\mu Q^j\big)\), for \(i,j=1,2,3\).
CHQ3_kk, CHQ3_klr, CHQ3_kli \( (C_{HQ}^{(3)})_{kk}, \mbox{Re}\big[(C_{HQ}^{(3)})_{kl}\big], \mbox{Im}\big[(C_{HQ}^{(3)})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HQ}^{(3)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{Q^i}\,\gamma^\mu \sigma^a Q^j\big)\), for \(i,j=1,2,3\).
CHu_kk, CHu_klr, CHu_kli \( (C_{Hu})_{kk}, \mbox{Re}\big[(C_{Hu})_{kl}\big], \mbox{Im}\big[(C_{Hu})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hu})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{U^i}\,\gamma^\mu U^j\big)\), for \(i,j=1,2,3\).
CHd_kk, CHd_klr, CHd_kli \( (C_{Hd})_{kk}, \mbox{Re}\big[(C_{Hd})_{kl}\big], \mbox{Im}\big[(C_{Hd})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hd})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{D^i}\,\gamma^\mu D^j\big)\), for \(i,j=1,2,3\).
CHud_klr, CHud_kli \(\mbox{Re}\big[(C_{Hud})_{kl}\big], \mbox{Im}\big[(C_{Hud})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hud})_{ij} =i\big(\widetilde{H}^\dagger D_\mu H\big) \big(\overline{U^i}\,\gamma^\mu D^j\big)\), for \(i,j=1,2,3\).
CeH_klr, CeH_kli \(\mbox{Re}\big[(C_{eH})_{kl}\big], \mbox{Im}\big[(C_{eH})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eH})_{ij} =\big(H^\dagger H\big) \big(\overline{L^i}\,H E^j\big)\), for \(i,j=1,2,3\).
CuH_klr, CuH_kli \(\mbox{Re}\big[(C_{uH})_{kl}\big], \mbox{Im}\big[(C_{uH})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uH})_{ij} =\big(H^\dagger H\big) \big(\overline{Q^i}\,\widetilde{H} U^j\big)\), for \(i,j=1,2,3\).
CdH_klr, CdH_kli \(\mbox{Re}\big[(C_{dH})_{kl}\big], \mbox{Im}\big[(C_{dH})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dH})_{ij} =\big(H^\dagger H\big) \big(\overline{Q^i}\,H D^j\big)\), for \(i,j=1,2,3\).
CuG_klr, CuG_kli \(\mbox{Re}\big[(C_{uG})_{kl}\big], \mbox{Im}\big[(C_{uG})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uG})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} T_A U^j\big)\widetilde{H} G_{\mu\nu}^A\), for \(i,j=1,2,3\).
CuW_klr, CuW_kli \(\mbox{Re}\big[(C_{uW})_{kl}\big], \mbox{Im}\big[(C_{uW})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uW})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} \sigma_a U^j\big)\widetilde{H} W_{\mu\nu}^a\), for \(i,j=1,2,3\).
CuB_klr, CuB_kli \(\mbox{Re}\big[(C_{uB})_{kl}\big], \mbox{Im}\big[(C_{uB})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uB})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} U^j\big)\widetilde{H} B_{\mu\nu}\), for \(i,j=1,2,3\).
CLL_1221, CLL_2112 \((C_{LL})_{1221,2112}\) The coefficient of the operator \(({\cal O}_{LL})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{L^k}\,\gamma_\mu L^l\big)\), for \(ijkl=1221,2112\).
CLQ1 \(C_{LQ}^{(1)}\) The coefficient of the operator \(({\cal O}_{LQ}^{(1)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{Q^k}\,\gamma_\mu Q^l\big)\).
CLQ3 \(C_{LQ}^{(3)}\) The coefficient of the operator \(({\cal O}_{LQ}^{(3)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu \sigma_a L^j\big) \big(\overline{Q^k}\,\gamma_\mu \sigma_a Q^l\big)\).
Cee \(C_{EE}\) The coefficient of the operator \(({\cal O}_{EE})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\).
Ceu \(C_{EU}\) The coefficient of the operator \(({\cal O}_{EU})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\).
Ced \(C_{ED}\) The coefficient of the operator \(({\cal O}_{ED})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\).
CLe \(C_{LE}\) The coefficient of the operator \(({\cal O}_{LE})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\).
CLu \(C_{LU}\) The coefficient of the operator \(({\cal O}_{LU})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\).
CLd \(C_{LD}\) The coefficient of the operator \(({\cal O}_{LD})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\).
CQe \(C_{QE}\) The coefficient of the operator \(({\cal O}_{QE})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\).
Lambda_NP \(\Lambda \) The new physics scale.
BrHinv Br \((H\to invisible)\) The branching ratio of invisible Higgs decays. Only the absolute value of this parameter is considered.(Not part of the EFT. Only for tests.)
BrHexo Br \((H\to exotic)\) The branching ratio of exotic Higgs decays. Only the absolute value of this parameter is considered. (Not part of the EFT. Only for tests.)
dg1Z \(\delta g_{1Z}\) Independent contribution to aTGC. (extra contribution to the one from the EFT. Only for tests.)
dKappaga \(\delta \kappa_{\gamma}\) Independent contribution to aTGC. (extra contribution to the one from the EFT. Only for tests.)
lambZ \(\lambda_{Z}\) Independent contribution to aTGC. (extra contribution to the one from the EFT. Only for tests.)
eXint \(\varepsilon_{X}^{int}\) The relative intrinsic theoretical uncertainty for the process X. (Only for Higgs observables and assumed to be constant in the energy.)
eXpar \(\varepsilon_{X}^{par}\) The relative parametric theoretical uncertainty for the process X. (Only for Higgs observables and assumed to be constant in the energy.)
eVBFE_i \(\varepsilon_{VBF}^i(E)\) The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the VBF production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i=g_{HZZ}^{(1,2,3)}, g_{HZA}^{(1,2)}, g_{HAA}, g_{HWW}^{(1,2,3)}, g_{Hgg}, g_{HZuu,HZdd}^{L,R}, g_{HWud}^{L}, g_{Zuu,Zdd}^{L,R}, g_{Wud}^{L})\)
eWHE_i \(\varepsilon_{WH}^i(E)\) The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the WH production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i= g_{HWW}^{(1,2,3)}, g_{HWud}^{L}, g_{Wud}^{L})\)
eZHE_i \(\varepsilon_{ZH}^i(E)\) The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the ZH production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i=g_{HZZ}^{(1,2,3)}, g_{HZA}^{(1,2)}, g_{HZuu,HZdd}^{L,R}, g_{Zuu,Zdd}^{L,R})\)
ettHE_i \(\varepsilon_{ttH}^i(E)\) The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the ttH production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i= g_{Htt}, g_{Hgg})\)

Where the hermitian derivatives are defined as

\[ H^\dagger i \overset{\leftrightarrow}{D}_\mu H\equiv H^\dagger i(D_\mu - \overset{\leftarrow}{D}_\mu)H \]

and

\[ H^\dagger i \overset{\leftrightarrow}{D^a_\mu} H\equiv H^\dagger i (\sigma^a D_\mu - \overset{\leftarrow}{D}_\mu \sigma^a)H. \]

Alternatively, when using the model name "NPSMEFTd6_LFU_QFU", where lepton and quark flavour universality are assumed (except for \((C_{fH})_{ij},~f=e,u,d\) which are assumed to be diagonal only), the parameters to be used as inputs for the dimension six coefficients are the following:

Label LaTeX symbol Description
CG \(C_{G} \) The coefficient of the operator \({\cal O}_{G}=f_{ABC}G_{\mu}^{A\nu} G_{\nu}^{B\rho}W_{\rho}^{C\mu}\).
CW \(C_{W} \) The coefficient of the operator \({\cal O}_{W}=\varepsilon_{abc}W_{\mu}^{a\nu} W_{\nu}^{b\rho}W_{\rho}^{b\mu}\).
C2B \(C_{2B} \) The coefficient of the operator \({\cal O}_{2B}=\frac 12 (\partial_\rho B_{\mu\nu})^2\). (Implemented via EOM.)
C2W \(C_{2W} \) The coefficient of the operator \({\cal O}_{2W}=\frac 12 (D_\rho W_{\mu\nu}^{a})^2\). (Implemented via EOM.)
C2BS \(C_{2B}^{SILH} \) The coefficient of the SILH operator \({\cal O}_{2B}^{SILH}=\frac 12 (\partial^\mu B_{\mu\nu})(\partial_\rho B^{\rho\nu})\). (Implemented via EOM.)
C2WS \(C_{2W}^{SILH} \) The coefficient of the operator \({\cal O}_{2W}^{SILH}=\frac 12 (D_\mu W^{a~\!\mu\nu})(D^\rho W_{\rho\nu}^{a})\). (Implemented via EOM.)
CHG \(C_{HG} \) The coefficient of the operator \({\cal O}_{HG}=\big(H^\dagger H\big)G_{\mu\nu}^A G^{A\mu\nu}\).
CHW \(C_{HW} \) The coefficient of the operator \({\cal O}_{HW}=\big(H^\dagger H\big)W_{\mu\nu}^a W^{a\mu\nu}\).
CHB \(C_{HB} \) The coefficient of the operator \({\cal O}_{HB}=\big(H^\dagger H\big)B_{\mu\nu} B^{\mu\nu}\).
CDHB \(C_{DHB} \) The coefficient of the operator \({\cal O}_{DHB}=i\big(D^\mu H^\dagger D^\nu H\big) B_{\mu\nu}\).
CDHW \(C_{DHW}\) The coefficient of the operator \({\cal O}_{DHW}=i\big(D^\mu H^\dagger \sigma^a D^\nu H\big) W_{\mu\nu}^a\).
CDB \(C_{DB} \) The coefficient of the operator \({\cal O}_{DB}=\frac{i}{2}\big(H^\dagger \overset{\leftrightarrow}{D}^\mu H\big) \partial^\nu B_{\mu\nu}\). (Implemented via EOM.)
CDW \(C_{DW}\) The coefficient of the operator \({\cal O}_{DW}=\frac{i}{2}\big(H^\dagger \overset{\leftrightarrow}{D}^{a~\!\mu} H\big) D^\nu W_{\mu\nu}^a\). (Implemented via EOM.)
CWB \(C_{WB} \) The coefficient of the operator \({\cal O}_{HWB}=\big(H^\dagger\sigma^a H\big)W_{\mu\nu}^a B^{\mu\nu}\).
CHD \(C_{HD}\) The coefficient of the operator \({\cal O}_{HD}=\big|H^\dagger D_\mu H\big|^2\).
CT \(C_{T}\) The coefficient of the operator \({\cal O}_{T}=\frac{1}{2} \big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big)^2\).
CHbox \(C_{H\Box}\) The coefficient of the operator \({\cal O}_{H\Box}=\big(H^\dagger H\big)\Box\big(H^\dagger H\big)\).
CH \(C_{H}\) The coefficient of the operator \({\cal O}_{H}=\big(H^\dagger H\big)^3\).
CHL1 \( (C_{HL}^{(1)})_{ii} \) The coefficient of the operator \(({\cal O}_{HL}^{(1)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{L^i}\,\gamma^\mu L^i\big)\) (flavor universal).
CHL3 \( (C_{HL}^{(3)})_{ii} \) The coefficient of the operator \(({\cal O}_{HL}^{(3)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{L^i}\,\gamma^\mu \sigma^a L^i\big)\) (flavor universal).
CHe \( (C_{He})_{ii} \) The coefficient of the operator \(({\cal O}_{He})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{E^i}\,\gamma^\mu E^i\big)\) (flavor universal).
CHQ1 \( (C_{HQ}^{(1)})_{ii} \) The coefficient of the operator \(({\cal O}_{HQ}^{(1)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{Q^i}\,\gamma^\mu Q^i\big)\) (flavor universal).
CHQ3 \( (C_{HQ}^{(3)})_{ii}\) The coefficient of the operator \(({\cal O}_{HQ}^{(3)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{Q^i}\,\gamma^\mu \sigma^a Q^i\big)\) (flavor universal).
CHu \( (C_{Hu})_{ii} \) The coefficient of the operator \(({\cal O}_{Hu})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{U^i}\,\gamma^\mu U^i\big)\) (flavor universal).
CHd \( (C_{Hd})_{ii} \) The coefficient of the operator \(({\cal O}_{Hd})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{D^i}\,\gamma^\mu D^i\big)\) (flavor universal).
CHud_r, CHud_i \(\mbox{Re}\big[(C_{Hud})_{ii}\big], \mbox{Im}\big[(C_{Hud})_{ii}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hud})_{ii} =i\big(\widetilde{H}^\dagger D_\mu H\big) \big(\overline{U^i}\,\gamma^\mu D^i\big)\) (flavor universal).
CeH_jjr, CeH_jji \(\mbox{Re}\big[(C_{eH})_{jj}\big], \mbox{Im}\big[(C_{eH})_{jj}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eH})_{jj} =\big(H^\dagger H\big) \big(\overline{L^j}\,H E^j\big)\) (flavor universal).
CuH_jjr, CuH_jji \(\mbox{Re}\big[(C_{uH})_{jj}\big], \mbox{Im}\big[(C_{uH})_{jj}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uH})_{jj} =\big(H^\dagger H\big) \big(\overline{Q^j}\,\widetilde{H} U^j\big)\) (flavor universal).
CdH_jjr, CdH_jji \(\mbox{Re}\big[(C_{dH})_{jj}\big], \mbox{Im}\big[(C_{dH})_{jj}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dH})_{jj} =\big(H^\dagger H\big) \big(\overline{Q^j}\,H D^j\big)\) (flavor universal).
CuG_klr, CuG_kli \(\mbox{Re}\big[(C_{uG})_{kl}\big], \mbox{Im}\big[(C_{uG})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uG})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} T_A U^j\big)\widetilde{H} G_{\mu\nu}^A\), for \(i,j=1,2,3\).
CuW_klr, CuW_kli \(\mbox{Re}\big[(C_{uW})_{kl}\big], \mbox{Im}\big[(C_{uW})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uW})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} \sigma_a U^j\big)\widetilde{H} W_{\mu\nu}^a\), for \(i,j=1,2,3\).
CuB_klr, CuB_kli \(\mbox{Re}\big[(C_{uB})_{kl}\big], \mbox{Im}\big[(C_{uB})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uB})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} U^j\big)\widetilde{H} B_{\mu\nu}\), for \(i,j=1,2,3\).
CLL \((C_{LL})_{1221,2112}\) The coefficient of the operator \(({\cal O}_{LL})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{L^k}\,\gamma_\mu L^l\big)\), for \(ijkl=1221,2112\).
CLQ1 \(C_{LQ}^{(1)}\) The coefficient of the operator \(({\cal O}_{LQ}^{(1)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{Q^k}\,\gamma_\mu Q^l\big)\).
CLQ3 \(C_{LQ}^{(3)}\) The coefficient of the operator \(({\cal O}_{LQ}^{(3)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu \sigma_a L^j\big) \big(\overline{Q^k}\,\gamma_\mu \sigma_a Q^l\big)\).
Cee \(C_{EE}\) The coefficient of the operator \(({\cal O}_{EE})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\).
Ceu \(C_{EU}\) The coefficient of the operator \(({\cal O}_{EU})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\).
Ced \(C_{ED}\) The coefficient of the operator \(({\cal O}_{ED})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\).
CLe \(C_{LE}\) The coefficient of the operator \(({\cal O}_{LE})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\).
CLu \(C_{LU}\) The coefficient of the operator \(({\cal O}_{LU})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\).
CLd \(C_{LD}\) The coefficient of the operator \(({\cal O}_{LD})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\).
CQe \(C_{QE}\) The coefficient of the operator \(({\cal O}_{QE})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\).
Lambda_NP \(\Lambda \) The new physics scale.
BrHinv Br \((H\to invisible)\) The branching ratio of invisible Higgs decays. (Not part of the EFT. Only for tests.)
BrHexo Br \((H\to exotic)\) The branching ratio of exotic Higgs decays. (Not part of the EFT. Only for tests.)

(The parameters associated to the theoretical uncertainties: \(\varepsilon_{X}^{int}\), \(\varepsilon_{X}^{par}\) and \(\varepsilon_{X}^i(E)\), are the same for both "NPSMEFTd6" and "NPSMEFTd6_LFU_QFU".)

Model flags

The Flags of NPSMEFTd6 are summarized below:

Label Value Description
QuadraticTerms TRUE / FALSE This flag is set to TRUE if the quadratic terms in Higgs cross sections and widths are switched on. The default value is FALSE; new physics contributions are linearized.
RotateCHWCHB TRUE / FALSE This flag is set to TRUE if using {sW2*CHW+cW2*CHB, -cW2*CHW+sW2*CHB} instead of {CHW, CHB} as floating parameters. The default value is FALSE.
PartialQFU TRUE / FALSE This flag is set to TRUE if using CHQ1_11=CHQ1_22, CHQ3_11=CHQ3_22, CHU_11=CHU_22, CHD_11=CHD_22, CHud_11=CHud_22.} Only applies in the Non QFU case. In that case only the (1,1) component is taken into account. The default value is FALSE.
FlavU3OfX TRUE / FALSE This flag is set to TRUE if using \(U(3)^5\) flavour symmetry relations in the coefficients of the operators \(O_{fH}\) and \(O_{fV}\). If TRUE, the operator coefficient is proportional to the corresponding Yukawa matrix (diagonal), with the proportionality coefficient given by the Model parameter corresponding to the coefficient of third family. (Implemented only for the real and diagonal elements of the \(O_{fH}\) and \(O_{fV}\) operators.) The default value is FALSE.
FlagUnivOfX TRUE / FALSE This flag is set to TRUE if using \(U(3)^5\) flavour symmetry relations in the coefficients of the operators \(O_{fH}\) and \(O_{fV}\) plus they are the same for all fermions. If TRUE, all the operator coefficients are proportional to the corresponding Yukawa matrix (diagonal), with the proportionality coefficient given by the Model parameter corresponding to the coefficients of third family for \(O_{uH}\) and \(O_{uV}\), respectively. (Implemented only for the real and diagonal elements of the \(O_{fH}\) and \(O_{fV}\) operators.) The default value is FALSE.
HiggsSM TRUE / FALSE This flag is set to TRUE if including dependence on small variations of the SM parameters (dependence is linearized). Available only in selected Higgs observables. The default value is FALSE.
LoopHd6 TRUE / FALSE This flag is set to TRUE if including modifications in the SM loops in Higgs observables due to the dim 6 interactions. The default value is FALSE.
LoopH3d6Quad TRUE / FALSE

This flag is set to TRUE if including quadratic modifications in the SM loops in Higgs observables due to the dim 6 interactions that contribute to the trilinear Higgs coupling. Works independently of the flag QuadraticTerms (the quadratic contributions are also added if the latter is true). The default value is FALSE.

Important member functions

See the base classes of the current class.

Definition at line 825 of file NPSMEFTd6.h.

Public Member Functions

gslpp::complex AH_f (const double tau) const
 Fermionic loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings. More...
 
gslpp::complex AH_W (const double tau) const
 W loop function entering in the calculation of the effective \(H\gamma\gamma\) coupling. More...
 
gslpp::complex AHZga_f (const double tau, const double lambda) const
 Fermionic loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More...
 
gslpp::complex AHZga_W (const double tau, const double lambda) const
 W loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More...
 
virtual double aPskPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 the angular parameter \(a\) from \(\mu_{e^+e^- \to ZH}\) (arXiv:1708.09079 [hep-ph]). More...
 
virtual double AuxObs_NP1 () const
 Auxiliary observable AuxObs_NP1 (See code for details.) More...
 
virtual double AuxObs_NP10 () const
 Auxiliary observable AuxObs_NP10 (See code for details.) More...
 
virtual double AuxObs_NP11 () const
 Auxiliary observable AuxObs_NP11 (See code for details.) More...
 
virtual double AuxObs_NP12 () const
 Auxiliary observable AuxObs_NP12 (See code for details.) More...
 
virtual double AuxObs_NP13 () const
 Auxiliary observable AuxObs_NP13. More...
 
virtual double AuxObs_NP14 () const
 Auxiliary observable AuxObs_NP14. More...
 
virtual double AuxObs_NP15 () const
 Auxiliary observable AuxObs_NP15. More...
 
virtual double AuxObs_NP16 () const
 Auxiliary observable AuxObs_NP16. More...
 
virtual double AuxObs_NP17 () const
 Auxiliary observable AuxObs_NP17. More...
 
virtual double AuxObs_NP18 () const
 Auxiliary observable AuxObs_NP18. More...
 
virtual double AuxObs_NP19 () const
 Auxiliary observable AuxObs_NP19. More...
 
virtual double AuxObs_NP2 () const
 Auxiliary observable AuxObs_NP2 (See code for details.) More...
 
virtual double AuxObs_NP20 () const
 Auxiliary observable AuxObs_NP20. More...
 
virtual double AuxObs_NP3 () const
 Auxiliary observable AuxObs_NP3 (See code for details.) More...
 
virtual double AuxObs_NP4 () const
 Auxiliary observable AuxObs_NP4 (See code for details.) More...
 
virtual double AuxObs_NP5 () const
 Auxiliary observable AuxObs_NP5 (See code for details.) More...
 
virtual double AuxObs_NP6 () const
 Auxiliary observable AuxObs_NP6 (See code for details.) More...
 
virtual double AuxObs_NP7 () const
 Auxiliary observable AuxObs_NP7 (See code for details.) More...
 
virtual double AuxObs_NP8 () const
 Auxiliary observable AuxObs_NP8 (See code for details.) More...
 
virtual double AuxObs_NP9 () const
 Auxiliary observable AuxObs_NP9 (See code for details.) More...
 
virtual double bPskPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 the angular parameter \(b\) from \(\mu_{e^+e^- \to ZH}\) (arXiv:1708.09079 [hep-ph]). More...
 
virtual double Br_H_exo () const
 The branching ratio of the of the Higgs into exotic particles. More...
 
virtual double Br_H_inv () const
 The branching ratio of the of the Higgs into invisible particles. More...
 
virtual double Br_H_inv_NP () const
 The branching ratio of the of the Higgs into invisible particles (only invisible new particles). More...
 
virtual double BrHbbRatio () const
 The ratio of the Br \((H\to b\bar{b})\) in the current model and in the Standard Model. More...
 
virtual double BrHccRatio () const
 The ratio of the Br \((H\to c\bar{c})\) in the current model and in the Standard Model. More...
 
virtual double BrHgagaRatio () const
 The ratio of the Br \((H\to \gamma\gamma)\) in the current model and in the Standard Model. More...
 
virtual double BrHggRatio () const
 The ratio of the Br \((H\to gg)\) in the current model and in the Standard Model. More...
 
virtual double BrHmumuRatio () const
 The ratio of the Br \((H\to \mu^+\mu^-)\) in the current model and in the Standard Model. More...
 
virtual double BrHtautauRatio () const
 The ratio of the Br \((H\to \tau^+\tau^-)\) in the current model and in the Standard Model. More...
 
virtual double BrHtoinvRatio () const
 The ratio of the Br \((H\to invisible)\) in the current model and in the Standard Model. More...
 
virtual double BrHvisRatio () const
 The ratio of the Br \((H\to visible)\) in the current model and in the Standard Model. More...
 
virtual double BrHWffRatio () const
 The ratio of the Br \((H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
virtual double BrHWjjRatio () const
 The ratio of the Br \((H\to W j j)\) in the current model and in the Standard Model. More...
 
virtual double BrHWlvRatio () const
 The ratio of the Br \((H\to W l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
virtual double BrHWW2l2vRatio () const
 The ratio of the Br \((H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
virtual double BrHWW4fRatio () const
 The ratio of the Br \((H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
virtual double BrHWW4jRatio () const
 The ratio of the Br \((H\to WW^*\to 4j)\) in the current model and in the Standard Model. More...
 
virtual double BrHWWRatio () const
 The ratio of the Br \((H\to WW)\) in the current model and in the Standard Model. More...
 
virtual double BrHZddRatio () const
 The ratio of the Br \((H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More...
 
virtual double BrHZffRatio () const
 The ratio of the Br \((H\to Zff)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
virtual double BrHZgaeeRatio () const
 The ratio of the Br \((H\to Z\gamma\to ee\gamma)\) in the current model and in the Standard Model. More...
 
virtual double BrHZgallRatio () const
 The ratio of the Br \((H\to Z\gamma\to ll\gamma)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
virtual double BrHZgamumuRatio () const
 The ratio of the Br \((H\to Z\gamma\to \mu\mu\gamma)\) in the current model and in the Standard Model. More...
 
virtual double BrHZgaRatio () const
 The ratio of the Br \((H\to Z\gamma)\) in the current model and in the Standard Model. More...
 
virtual double BrHZllRatio () const
 The ratio of the Br \((H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
virtual double BrHZuuRatio () const
 The ratio of the Br \((H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More...
 
virtual double BrHZvvRatio () const
 The ratio of the Br \((H\to Z\nu\nu)\) in the current model and in the Standard Model. More...
 
virtual double BrHZZ2e2muRatio () const
 The ratio of the Br \((H\to ZZ* \to 2e 2\mu)\) in the current model and in the Standard Model. More...
 
virtual double BrHZZ4dRatio () const
 The ratio of the Br \((H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More...
 
virtual double BrHZZ4eRatio () const
 The ratio of the Br \((H\to ZZ* \to 4e)\) in the current model and in the Standard Model. More...
 
virtual double BrHZZ4fRatio () const
 The ratio of the Br \((H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
virtual double BrHZZ4lRatio () const
 The ratio of the Br \((H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
virtual double BrHZZ4muRatio () const
 The ratio of the Br \((H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. More...
 
virtual double BrHZZ4uRatio () const
 The ratio of the Br \((H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More...
 
virtual double BrHZZ4vRatio () const
 The ratio of the Br \((H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. More...
 
virtual double BrHZZRatio () const
 The ratio of the Br \((H\to ZZ)\) in the current model and in the Standard Model. More...
 
virtual double cgaga_HB () const
 The Higgs-basis coupling \(c_{\gamma\gamma}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double cgg_HB () const
 The Higgs-basis coupling \(c_{gg}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double cggEff_HB () const
 The effective Higgs-basis coupling \(c_{gg}^{Eff}\). (Similar to cgg_HB but including modifications of SM loops.) (See arXiv: 1505.00046 [hep-ph] document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual bool CheckParameters (const std::map< std::string, double > &DPars)
 A method to check if all the mandatory parameters for NPSMEFTd6 have been provided in model initialization. More...
 
double CLL_bottom () const
 
double CLL_charm () const
 
double CLL_down () const
 
double CLL_mu () const
 
double CLL_strange () const
 
double CLL_tau () const
 
double CLL_up () const
 
double CLR_bottom () const
 
double CLR_charm () const
 
double CLR_down () const
 
double CLR_mu () const
 
double CLR_strange () const
 
double CLR_tau () const
 
double CLR_up () const
 
virtual double computeGammaTotalRatio () const
 The ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. More...
 
double CRL_bottom () const
 
double CRL_charm () const
 
double CRL_down () const
 
double CRL_mu () const
 
double CRL_strange () const
 
double CRL_tau () const
 
double CRL_up () const
 
double CRR_bottom () const
 
double CRR_charm () const
 
double CRR_down () const
 
double CRR_mu () const
 
double CRR_strange () const
 
double CRR_tau () const
 
double CRR_up () const
 
virtual double cZBox_HB () const
 The Higgs-basis coupling \(c_{z\Box}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double cZga_HB () const
 The Higgs-basis coupling \(c_{z\gamma}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double cZZ_HB () const
 The Higgs-basis coupling \(c_{zz}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double deltaa0 () const
 The relative correction to the electromagnetic constant at zero momentum, \(\delta \alpha(0)/\alpha(0)\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltaa02 () const
 The relative correction to the electromagnetic constant at zero momentum, \((\delta \alpha(0)/\alpha(0))^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltaaMZ () const
 The relative correction to the electromagnetic constant at the Z pole, \(\delta \alpha(M_Z^2)/\alpha(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltaaMZ2 () const
 The relative correction to the electromagnetic constant at the Z pole, \((\delta \alpha(M_Z^2)/\alpha(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltaaSMZ () const
 The relative correction to the strong coupling constant at the Z pole, \(\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltaaSMZ2 () const
 The relative correction to the strong coupling constant at the Z pole, \((\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltacZ_HB () const
 The Higgs-basis coupling \(\delta c_z\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double deltaG1_hWW () const
 The new physics contribution to the coupling of the effective interaction \(H W_{\mu\nu}^\dagger W^{\mu\nu}\). More...
 
virtual double deltaG1_hZA () const
 The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{\mu\nu}\). More...
 
virtual double deltaG1_hZARatio () const
 The full new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More...
 
virtual double deltaG1_hZZ () const
 The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} Z^{\mu\nu}\). More...
 
virtual double deltag1ZNP () const
 The new physics contribution to the anomalous triple gauge coupling \(g_{1,Z}\). More...
 
virtual double deltag1ZNPEff () const
 The new physics contribution to the effective anomalous triple gauge coupling \(g_{1,Z}^{Eff}\) from arXiv: 1708.09079 [hep-ph]. More...
 
virtual double deltaG2_hWW () const
 The new physics contribution to the coupling of the effective interaction \(H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}\). More...
 
virtual double deltaG2_hZA () const
 The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu F^{\mu\nu}\). More...
 
virtual double deltaG2_hZZ () const
 The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu Z^{\mu\nu}\). More...
 
virtual double deltaG3_hWW () const
 The new physics contribution to the coupling of the effective interaction \(H W_{\mu}^\dagger W^{\mu}\). More...
 
virtual double deltaG3_hZZ () const
 The new physics contribution to the coupling of the effective interaction \(H Z_{\mu} Z^{\mu}\). More...
 
double deltag3G () const
 The new physics contribution to the coupling of the effective interaction \(f_{ABC} G_{\mu\nu}^A G_{\nu\rho}^B G_{\rho\mu}^C\). More...
 
gslpp::complex deltaG_Aff (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More...
 
gslpp::complex deltaG_Gff (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(G_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More...
 
virtual double deltaG_hAA () const
 The new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\). More...
 
virtual double deltaG_hAARatio () const
 The full new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More...
 
gslpp::complex deltaG_hAff (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More...
 
virtual gslpp::complex deltaG_hff (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H f\bar{f}\). More...
 
gslpp::complex deltaG_hGff (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More...
 
virtual double deltaG_hgg () const
 The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\). More...
 
virtual double deltaG_hggRatio () const
 The full new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More...
 
virtual double deltaG_hhhRatio () const
 The new physics contribution to the Higgs self-coupling \( H H H\). Normalized to the SM value. More...
 
gslpp::complex deltaG_hZff (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More...
 
gslpp::complex deltaG_Zff (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(Z_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More...
 
virtual double deltaGA_f (const Particle p) const
 New physics contribution to the neutral-current axial-vector coupling \(g_A^f\). More...
 
virtual double deltaGamma_W () const
 The new physics contribution to the total decay width of the \(W\) boson, \(\delta \Gamma_W\). More...
 
virtual double deltaGamma_Wff (const Particle fi, const Particle fj) const
 The new physics contribution to the decay width of the \(W\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\). More...
 
double deltaGammaHbbRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHbbRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHccRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHccRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHgagaRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHgagaRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHggRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. More...
 
double deltaGammaHggRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHmumuRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHmumuRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHtautauRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHtautauRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWffRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWffRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWjjRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWjjRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWlvRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Wl\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWlvRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Wl\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWW2l2vRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWW2l2vRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWW4fRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWW4fRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWW4jRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWW4jRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWWRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWWRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZddRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZddRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZeeRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZeeRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZffRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z ff)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZffRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z ff)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZgaRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZgaRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZllRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZllRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZmumuRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZmumuRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZuuRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZuuRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZvvRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZvvRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ2e2muRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ2e2muRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4dRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4dRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4eRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4eRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4fRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4fRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4lRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4lRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4muRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4muRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4uRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4uRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4vRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4vRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
virtual double deltaGammaTotalRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. More...
 
virtual double deltaGammaTotalRatio1noError () const
 The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. Neglecting SM theory errors. More...
 
virtual double deltaGammaTotalRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are quadratic in the effective Lagrangian coefficients. More...
 
virtual double DeltaGF () const
 New physics contribution to the Fermi constant. More...
 
double deltaGL_f (const Particle p) const
 New physics contribution to the neutral-current left-handed coupling \(g_L^f\). More...
 
virtual gslpp::complex deltaGL_Wff (const Particle pbar, const Particle p) const
 New physics contribution to the charged current coupling \(W_\mu \bar{f_L}\gamma^mu f_L\). More...
 
gslpp::complex deltaGL_Wffh (const Particle pbar, const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_L}\gamma^mu f_L\). More...
 
double deltaGL_Zffh (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_L}\gamma^mu f_L\). More...
 
virtual double deltaGmu () const
 The relative correction to the muon decay constant, \(\delta G_\mu/G_\mu\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltaGmu2 () const
 The relative correction to the muon decay constant, \((\delta G_\mu/G_\mu)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
double deltaGR_f (const Particle p) const
 New physics contribution to the neutral-current right-handed coupling \(g_R^f\). More...
 
virtual gslpp::complex deltaGR_Wff (const Particle pbar, const Particle p) const
 New physics contribution to the charged current coupling \(W_\mu \bar{f_R}\gamma^mu f_R\). More...
 
gslpp::complex deltaGR_Wffh (const Particle pbar, const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_R}\gamma^mu f_R\). More...
 
double deltaGR_Zffh (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_R}\gamma^mu f_R\). More...
 
virtual double deltaGV_f (const Particle p) const
 New physics contribution to the neutral-current vector coupling \(g_V^f\). More...
 
virtual double deltaGwd6 () const
 The relative NP corrections to the width of the \(W\) boson, \(\delta \Gamma_W/\Gamma_W\). More...
 
virtual double deltaGwd62 () const
 The relative NP corrections to the width of the \(W\) boson squared, \((\delta \Gamma_W/\Gamma_W)^2\). More...
 
virtual double deltaGzd6 () const
 The relative NP corrections to the width of the \(Z\) boson, \(\delta \Gamma_Z/\Gamma_Z\). More...
 
virtual double deltaGzd62 () const
 The relative NP corrections to the width of the \(Z\) boson squared, \((\delta \Gamma_Z/\Gamma_Z)^2\). More...
 
virtual double deltaKgammaNP () const
 The new physics contribution to the anomalous triple gauge coupling \(\kappa_{\gamma}\). More...
 
virtual double deltaKgammaNPEff () const
 The new physics contribution to the effective anomalous triple gauge coupling \(\kappa_{\gamma}^{Eff}\) from arXiv: 1708.09079 [hep-ph]. More...
 
virtual double deltamb () const
 The relative correction to the mass of the \(b\) quark, \(\delta m_b/m_b\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltamb2 () const
 The relative correction to the mass of the \(b\) quark squared, \((\delta m_b/m_b)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltamc () const
 The relative correction to the mass of the \(c\) quark, \(\delta m_c/m_c\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltamc2 () const
 The relative correction to the mass of the \(c\) quark squared, \((\delta m_c/m_c)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltaMh () const
 The relative correction to the mass of the \(H\) boson, \(\delta M_H/M_H\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltaMh2 () const
 The relative correction to the mass of the \(H\) boson squared, \((\delta M_H/M_H)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltamt () const
 The relative correction to the mass of the \(t\) quark, \(\delta m_t/m_t\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltamt2 () const
 The relative correction to the mass of the \(t\) quark squared, \((\delta m_t/m_t)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltamtau () const
 The relative correction to the mass of the \(\tau\) lepton, \(\delta m_\tau/m_\tau\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltamtau2 () const
 The relative correction to the mass of the \(\tau\) lepton squared, \((\delta m_\tau/m_\tau)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltaMwd6 () const
 The relative NP corrections to the mass of the \(W\) boson, \(\delta M_W/M_W\). More...
 
virtual double deltaMwd62 () const
 The relative NP corrections to the mass of the \(W\) boson squared, \((\delta M_W/M_W)^2\). More...
 
virtual double deltaMz () const
 The relative correction to the mass of the \(Z\) boson, \(\delta M_Z/M_Z\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltaMz2 () const
 The relative correction to the mass of the \(Z\) boson squared, \((\delta M_Z/M_Z)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltayb_HB () const
 The Higgs-basis coupling \(\delta y_b\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double deltayc_HB () const
 The Higgs-basis coupling \(\delta y_c\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double deltaymu_HB () const
 The Higgs-basis coupling \(\delta y_\mu\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double deltayt_HB () const
 The Higgs-basis coupling \(\delta y_t\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double deltaytau_HB () const
 The Higgs-basis coupling \(\delta y_\tau\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double dxseeWWdcos (const double sqrt_s, const double cos) const
 The differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\), as a function of the \(W\) polar angle. More...
 
virtual double dxseeWWdcosBin (const double sqrt_s, const double cos1, const double cos2) const
 The integral of differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\) in a given bin of the \(W\) polar angle. More...
 
gslpp::complex f_triangle (const double tau) const
 Loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings. More...
 
gslpp::complex g_triangle (const double tau) const
 Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More...
 
double GammaHbbRatio () const
 The ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. More...
 
double GammaHccRatio () const
 The ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. More...
 
double GammaHgagaRatio () const
 The ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. More...
 
double GammaHggRatio () const
 The ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. More...
 
double GammaHmumuRatio () const
 The ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. More...
 
double GammaHtautauRatio () const
 The ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. More...
 
double GammaHWffRatio () const
 The ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
double GammaHWjjRatio () const
 The ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. More...
 
double GammaHWlvRatio () const
 The ratio of the \(\Gamma(H\to W l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
double GammaHWW2l2vRatio () const
 The ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
double GammaHWW4fRatio () const
 The ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
double GammaHWW4jRatio () const
 The ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. More...
 
double GammaHWWRatio () const
 The ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. More...
 
double GammaHZddRatio () const
 The ratio of the \(\Gamma(H\to Zd d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More...
 
double GammaHZeeRatio () const
 The ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. More...
 
double GammaHZffRatio () const
 The ratio of the \(\Gamma(H\to Zff)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
double GammaHZgaRatio () const
 The ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. More...
 
double GammaHZllRatio () const
 The ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
double GammaHZmumuRatio () const
 The ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. More...
 
double GammaHZuuRatio () const
 The ratio of the \(\Gamma(H\to Zu u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More...
 
double GammaHZvvRatio () const
 The ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. More...
 
double GammaHZZ2e2muRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. More...
 
double GammaHZZ4dRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More...
 
double GammaHZZ4eRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. More...
 
double GammaHZZ4fRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
double GammaHZZ4lRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
double GammaHZZ4muRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. More...
 
double GammaHZZ4uRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More...
 
double GammaHZZ4vRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. More...
 
double GammaHZZRatio () const
 The ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. More...
 
virtual double GammaW () const
 The total width of the \(W\) boson, \(\Gamma_W\). More...
 
virtual double GammaW (const Particle fi, const Particle fj) const
 A partial decay width of the \(W\) boson decay into a SM fermion pair. More...
 
double getCed_1123 () const
 Return NP coeff Ced_1123. More...
 
double getCed_2223 () const
 Return NP coeff Ced_2223. More...
 
double getCeu_1133 () const
 Return NP coeff Ceu_1133. More...
 
double getCeu_2233 () const
 Return NP coeff Ceu_2233. More...
 
double getCHe_11 () const
 Return NP coeff CHe_11. More...
 
double getCHe_22 () const
 Return NP coeff CHe_22. More...
 
double getCHL1_11 () const
 Return NP coeff CHL1_11. More...
 
double getCHL1_22 () const
 Return NP coeff CHL1_22. More...
 
double getCHL3_11 () const
 Return NP coeff CHL3_11. More...
 
double getCHL3_22 () const
 Return NP coeff CHL3_22. More...
 
double getCLd_1123 () const
 Return NP coeff CLd_1123. More...
 
double getCLd_2223 () const
 Return NP coeff CLd_2223. More...
 
double getCLedQ_11 () const
 Return NP coeff CLedq_11. More...
 
double getCLedQ_22 () const
 Return NP coeff CLedq_22. More...
 
double getCLQ1_1123 () const
 Return NP coeff CLQ1_1123. More...
 
double getCLQ1_2223 () const
 Return NP coeff CLQ1_2223. More...
 
double getCLQ3_1123 () const
 Return NP coeff CLQ3_1123. More...
 
double getCLQ3_2223 () const
 Return NP coeff CLQ3_2223. More...
 
double getCLu_1133 () const
 Return NP coeff CLu_1133. More...
 
double getCLu_2233 () const
 Return NP coeff CLu_2233. More...
 
double getCpLedQ_11 () const
 Return NP coeff CpLedq_11. More...
 
double getCpLedQ_22 () const
 Return NP coeff CpLedq_22. More...
 
double getCQe_2311 () const
 Return NP coeff CQe_2322. More...
 
double getCQe_2322 () const
 Return NP coeff CQe_2322. More...
 
double getLambda_NP () const
 Return Lambda_NP. More...
 
virtual NPSMEFTd6MatchinggetMatching () const
 A method to get the Matching object for this model. More...
 
gslpp::complex I_triangle_1 (const double tau, const double lambda) const
 Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More...
 
gslpp::complex I_triangle_2 (const double tau, const double lambda) const
 Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More...
 
virtual double kappaAeff () const
 The effective coupling \(\kappa_{A,eff}=\sqrt{\Gamma_{HAA}/\Gamma_{HAA}^{SM}}\). More...
 
virtual double kappabeff () const
 The effective coupling \(\kappa_{b,eff}=\sqrt{\Gamma_{Hbb}/\Gamma_{Hbb}^{SM}}\). More...
 
virtual double kappaceff () const
 The effective coupling \(\kappa_{c,eff}=\sqrt{\Gamma_{Hcc}/\Gamma_{Hcc}^{SM}}\). More...
 
virtual double kappaGeff () const
 The effective coupling \(\kappa_{G,eff}=\sqrt{\Gamma_{HGG}/\Gamma_{HGG}^{SM}}\). More...
 
virtual double kappamueff () const
 The effective coupling \(\kappa_{\mu,eff}=\sqrt{\Gamma_{H\mu\mu}/\Gamma_{H\mu\mu}^{SM}}\). More...
 
virtual double kappataueff () const
 The effective coupling \(\kappa_{\tau,eff}=\sqrt{\Gamma_{H\tau\tau}/\Gamma_{H\tau\tau}^{SM}}\). More...
 
virtual double kappaWeff () const
 The effective coupling \(\kappa_{W,eff}=\sqrt{\Gamma_{HWW}/\Gamma_{HWW}^{SM}}\). More...
 
virtual double kappaZAeff () const
 The effective coupling \(\kappa_{ZA,eff}=\sqrt{\Gamma_{HZA}/\Gamma_{HZA}^{SM}}\). More...
 
virtual double kappaZeff () const
 The effective coupling \(\kappa_{Z,eff}=\sqrt{\Gamma_{HZZ}/\Gamma_{HZZ}^{SM}}\). More...
 
virtual double lambdaZNP () const
 The new physics contribution to the anomalous triple gauge coupling \(\lambda_{Z}\). More...
 
virtual double lambz_HB () const
 The Higgs-basis coupling \(\lambda_{z}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double mueeHvv (const double sqrt_s) const
 The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeHvvPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model. More...
 
virtual double mueettH (const double sqrt_s) const
 The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model. More...
 
virtual double mueettHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeWBF (const double sqrt_s) const
 The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeWBFPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeWW (const double sqrt_s) const
 The ratio \(\mu_{eeWW}\) between the \( e^{+}e^{-}\to W^{+}W^{-} \) production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeWWPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{eeWW}\) between the \( e^{+}e^{-}\to W^{+}W^{-} \) production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeZBF (const double sqrt_s) const
 The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeZBFPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeZH (const double sqrt_s) const
 The ratio \(\mu_{eeZH}\) between the \(e^{+}e^{-}\to ZH\) associated production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeZHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{eeZH}\) between the \( e^{+}e^{-}\to ZH \) associated production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeZllH (const double sqrt_s) const
 The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeZllHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeZqqH (const double sqrt_s) const
 The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeZqqHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model. More...
 
virtual double muepWBF (const double sqrt_s) const
 The ratio \(\mu_{epWBF}\) between the \( e^{-} p\to \nu j H \) production cross-section in the current model and in the Standard Model. More...
 
virtual double muepZBF (const double sqrt_s) const
 The ratio \(\mu_{epZBF}\) between the \( e^{-} p\to e^{-} j H \) production cross-section in the current model and in the Standard Model. More...
 
virtual double muggH (const double sqrt_s) const
 The ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model. More...
 
virtual double muggHbb (const double sqrt_s) const
 The ratio \(\mu_{ggH,bb}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual double muggHgaga (const double sqrt_s) const
 The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual double muggHH (const double sqrt_s) const
 The ratio \(\mu_{ggHH}\) between the gluon-gluon fusion di-Higgs production cross-section in the current model and in the Standard Model. (From arXiv: 1502.00539 [hpe-ph].) More...
 
virtual double muggHmumu (const double sqrt_s) const
 The ratio \(\mu_{ggH,\mu\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual double muggHpttH (const double sqrt_s) const
 The ratio \(\mu_{ggH+ttH}\) between the sum of gluon-gluon fusion and t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More...
 
virtual double muggHtautau (const double sqrt_s) const
 The ratio \(\mu_{ggH,\tau\tau}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual double muggHWW (const double sqrt_s) const
 The ratio \(\mu_{ggH,WW}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual double muggHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{ggH,WW\to 2l2\nu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual double muggHZga (const double sqrt_s) const
 The ratio \(\mu_{ggH,Z\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual double muggHZZ (const double sqrt_s) const
 The ratio \(\mu_{ggH,ZZ}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual double muggHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{ggH,ZZ\to 4l}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual double mummH (const double sqrt_s) const
 The ratio \(\mu_{\mu\mu H}\) between the \(\sigma(\mu \mu \to H)}\) production cross-section in the current model and in the Standard Model. More...
 
virtual double mupTVppWZ (const double sqrt_s, const double pTV1, const double pTV2) const
 The number of events in \( p p \to WZ\) in a given \(p_{TV}\) bin, normalized to the SM prediction. From arXiv: 1712.01310 [hep-ph] and private communication. Implemented only in NPSMEFTd6 class. More...
 
virtual double mutHq (const double sqrt_s) const
 The ratio \(\mu_{tHq}\) between the t-q-Higgs associated production cross-section in the current model and in the Standard Model. More...
 
virtual double muTHUggHbb (const double sqrt_s) const
 The ratio \(\mu_{ggH,bb}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual double muTHUggHgaga (const double sqrt_s) const
 The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual double muTHUggHmumu (const double sqrt_s) const
 The ratio \(\mu_{ggH,\mu\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual double muTHUggHtautau (const double sqrt_s) const
 The ratio \(\mu_{ggH,\tau\tau}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual double muTHUggHWW (const double sqrt_s) const
 The ratio \(\mu_{ggH,WW}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual double muTHUggHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{ggH,WW\to 2l2\nu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual double muTHUggHZga (const double sqrt_s) const
 The ratio \(\mu_{ggH,Z\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual double muTHUggHZgamumu (const double sqrt_s) const
 The ratio \(\mu_{ggH,Z\gamma\to \gamma 2\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\to \gamma 2\mu\) in the current model and in the Standard Model. More...
 
virtual double muTHUggHZZ (const double sqrt_s) const
 The ratio \(\mu_{ggH,ZZ}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual double muTHUggHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{ggH,ZZ\to 4l}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual double muTHUggHZZ4mu (const double sqrt_s) const
 The ratio \(\mu_{ggH,ZZ\to 4\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4\mu\) in the current model and in the Standard Model. More...
 
virtual double muTHUttHbb (const double sqrt_s) const
 The ratio \(\mu_{ttH,bb}\) between the ttH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual double muTHUttHgaga (const double sqrt_s) const
 The ratio \(\mu_{ttH,\gamma\gamma}\) between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual double muTHUttHmumu (const double sqrt_s) const
 The ratio \(\mu_{ttH,\mu\mu}\) between the ttH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual double muTHUttHtautau (const double sqrt_s) const
 The ratio \(\mu_{ttH,\tau\tau}\) between the ttH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual double muTHUttHWW (const double sqrt_s) const
 The ratio \(\mu_{ttH,WW}\) between the ttH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual double muTHUttHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{ttH,WW\to 2l2\nu}\) between the ttH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual double muTHUttHZga (const double sqrt_s) const
 The ratio \(\mu_{ttH,Z\gamma}\) between the ttH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual double muTHUttHZZ (const double sqrt_s) const
 The ratio \(\mu_{ttH,ZZ}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual double muTHUttHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{ttH,ZZ\to 4l}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual double muTHUVBFBRinv (const double sqrt_s) const
 The ratio \(\mu_{VBF}\) between the VBF production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio. More...
 
virtual double muTHUVBFHbb (const double sqrt_s) const
 The ratio \(\mu_{VBF,bb}\) between the VBF Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual double muTHUVBFHgaga (const double sqrt_s) const
 The ratio \(\mu_{VBF,\gamma\gamma}\) between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual double muTHUVBFHinv (const double sqrt_s) const
 The ratio \(\mu_{VBF,inv}\) between the VBF production cross-section with subsequent decay into invisible states in the current model and in the Standard Model. More...
 
virtual double muTHUVBFHmumu (const double sqrt_s) const
 The ratio \(\mu_{VBF,\mu\mu}\) between the VBF Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual double muTHUVBFHtautau (const double sqrt_s) const
 The ratio \(\mu_{VBF,\tau\tau}\) between the VBF Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual double muTHUVBFHWW (const double sqrt_s) const
 The ratio \(\mu_{VBF,WW}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual double muTHUVBFHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{VBF,WW\to 2l2\nu}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual double muTHUVBFHZga (const double sqrt_s) const
 The ratio \(\mu_{VBF,Z\gamma}\) between the VBF Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual double muTHUVBFHZZ (const double sqrt_s) const
 The ratio \(\mu_{VBF,ZZ}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual double muTHUVBFHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{VBF,ZZ\to 4l}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual double muTHUVHbb (const double sqrt_s) const
 The ratio \(\mu_{VH,bb}\) between the VH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual double muTHUVHBRinv (const double sqrt_s) const
 The ratio \(\mu_{VH}\) between the VH production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio. More...
 
virtual double muTHUVHgaga (const double sqrt_s) const
 The ratio \(\mu_{VH,\gamma\gamma}\) between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual double muTHUVHinv (const double sqrt_s) const
 The ratio \(\mu_{VH,inv}\) between the VH production cross-section with subsequent decay into invisible states in the current model and in the Standard Model. More...
 
virtual double muTHUVHmumu (const double sqrt_s) const
 The ratio \(\mu_{VH,\mu\mu}\) between the VH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual double muTHUVHtautau (const double sqrt_s) const
 The ratio \(\mu_{VH,\tau\tau}\) between the VH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual double muTHUVHWW (const double sqrt_s) const
 The ratio \(\mu_{VH,WW}\) between the VH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual double muTHUVHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{VH,WW\to 2l2\nu}\) between the VH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual double muTHUVHZga (const double sqrt_s) const
 The ratio \(\mu_{VH,Z\gamma}\) between the VH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual double muTHUVHZZ (const double sqrt_s) const
 The ratio \(\mu_{VH,ZZ}\) between the VH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual double muTHUVHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{VH,ZZ\to 4l}\) between the VH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual double muTHUWHbb (const double sqrt_s) const
 The ratio \(\mu_{WH,bb}\) between the WH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual double muTHUWHgaga (const double sqrt_s) const
 The ratio \(\mu_{WH,\gamma\gamma}\) between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual double muTHUWHmumu (const double sqrt_s) const
 The ratio \(\mu_{WH,\mu\mu}\) between the WH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual double muTHUWHtautau (const double sqrt_s) const
 The ratio \(\mu_{WH,\tau\tau}\) between the WH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual double muTHUWHWW (const double sqrt_s) const
 The ratio \(\mu_{WH,WW}\) between the WH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual double muTHUWHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{WH,WW\to 2l2\nu}\) between the WH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual double muTHUWHZga (const double sqrt_s) const
 The ratio \(\mu_{WH,Z\gamma}\) between the WH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual double muTHUWHZZ (const double sqrt_s) const
 The ratio \(\mu_{WH,ZZ}\) between the WH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual double muTHUWHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{WH,ZZ\to 4l}\) between the WH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual double muTHUZHbb (const double sqrt_s) const
 The ratio \(\mu_{ZH,bb}\) between the ZH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual double muTHUZHgaga (const double sqrt_s) const
 The ratio \(\mu_{ZH,\gamma\gamma}\) between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual double muTHUZHmumu (const double sqrt_s) const
 The ratio \(\mu_{ZH,\mu\mu}\) between the ZH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual double muTHUZHtautau (const double sqrt_s) const
 The ratio \(\mu_{ZH,\tau\tau}\) between the ZH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual double muTHUZHWW (const double sqrt_s) const
 The ratio \(\mu_{ZH,WW}\) between the ZH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual double muTHUZHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{ZH,WW\to 2l2\nu}\) between the ZH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual double muTHUZHZga (const double sqrt_s) const
 The ratio \(\mu_{ZH,Z\gamma}\) between the ZH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual double muTHUZHZZ (const double sqrt_s) const
 The ratio \(\mu_{ZH,ZZ}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual double muTHUZHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{ZH,ZZ\to 4l}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual double muttH (const double sqrt_s) const
 The ratio \(\mu_{ttH}\) between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More...
 
virtual double muttHbb (const double sqrt_s) const
 The ratio \(\mu_{ttH,bb}\) between the ttH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual double muttHgaga (const double sqrt_s) const
 The ratio \(\mu_{ttH,\gamma\gamma}\) between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual double muttHmumu (const double sqrt_s) const
 The ratio \(\mu_{ttH,\mu\mu}\) between the ttH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual double muttHtautau (const double sqrt_s) const
 The ratio \(\mu_{ttH,\tau\tau}\) between the ttH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual double muttHWW (const double sqrt_s) const
 The ratio \(\mu_{ttH,WW}\) between the ttH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual double muttHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{ttH,WW\to 2l2\nu}\) between the ttH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual double muttHZbbboost (const double sqrt_s) const
 The ratio \(\sigma(ttH)/\sigma(ttZ)\) in the \(H,Z\to b\bar{b}\) channel in the current model and in the Standard Model. More...
 
virtual double muttHZga (const double sqrt_s) const
 The ratio \(\mu_{ttH,Z\gamma}\) between the ttH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual double muttHZZ (const double sqrt_s) const
 The ratio \(\mu_{ttH,ZZ}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual double muttHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{ttH,ZZ\to 4l}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual double muVBF (const double sqrt_s) const
 The ratio \(\mu_{VBF}\) between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model. More...
 
virtual double muVBFgamma (const double sqrt_s) const
 The ratio \(\mu_{VBF+\gamma}\) between the vector-boson fusion Higgs production cross-section in association with a hard photon in the current model and in the Standard Model. More...
 
virtual double muVBFHbb (const double sqrt_s) const
 The ratio \(\mu_{VBF,bb}\) between the VBF Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual double muVBFHgaga (const double sqrt_s) const
 The ratio \(\mu_{VBF,\gamma\gamma}\) between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual double muVBFHmumu (const double sqrt_s) const
 The ratio \(\mu_{VBF,\mu\mu}\) between the VBF Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual double muVBFHtautau (const double sqrt_s) const
 The ratio \(\mu_{VBF,\tau\tau}\) between the VBF Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual double muVBFHWW (const double sqrt_s) const
 The ratio \(\mu_{VBF,WW}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual double muVBFHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{VBF,WW\to 2l2\nu}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual double muVBFHZga (const double sqrt_s) const
 The ratio \(\mu_{VBF,Z\gamma}\) between the VBF Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual double muVBFHZZ (const double sqrt_s) const
 The ratio \(\mu_{VBF,ZZ}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual double muVBFHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{VBF,ZZ\to 4l}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual double muVBFpVH (const double sqrt_s) const
 The ratio \(\mu_{VBF+VH}\) between the sum of VBF and WH+ZH associated production cross-section in the current model and in the Standard Model. More...
 
virtual double muVH (const double sqrt_s) const
 The ratio \(\mu_{VH}\) between the WH+ZH associated production cross-section in the current model and in the Standard Model. More...
 
virtual double muVHbb (const double sqrt_s) const
 The ratio \(\mu_{VH,bb}\) between the VH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual double muVHgaga (const double sqrt_s) const
 The ratio \(\mu_{VH,\gamma\gamma}\) between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual double muVHmumu (const double sqrt_s) const
 The ratio \(\mu_{VH,\mu\mu}\) between the VH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual double muVHtautau (const double sqrt_s) const
 The ratio \(\mu_{VH,\tau\tau}\) between the VH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual double muVHWW (const double sqrt_s) const
 The ratio \(\mu_{VH,WW}\) between the VH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual double muVHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{VH,WW\to 2l2\nu}\) between the VH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual double muVHZga (const double sqrt_s) const
 The ratio \(\mu_{VH,Z\gamma}\) between the VH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual double muVHZZ (const double sqrt_s) const
 The ratio \(\mu_{VH,ZZ}\) between the VH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual double muVHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{VH,ZZ\to 4l}\) between the VH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual double muWH (const double sqrt_s) const
 The ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model. More...
 
virtual double muWHbb (const double sqrt_s) const
 The ratio \(\mu_{WH,bb}\) between the WH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual double muWHgaga (const double sqrt_s) const
 The ratio \(\mu_{WH,\gamma\gamma}\) between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual double muWHmumu (const double sqrt_s) const
 The ratio \(\mu_{WH,\mu\mu}\) between the WH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual double muWHtautau (const double sqrt_s) const
 The ratio \(\mu_{WH,\tau\tau}\) between the WH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual double muWHWW (const double sqrt_s) const
 The ratio \(\mu_{WH,WW}\) between the WH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual double muWHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{WH,WW\to 2l2\nu}\) between the WH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual double muWHZga (const double sqrt_s) const
 The ratio \(\mu_{WH,Z\gamma}\) between the WH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual double muWHZZ (const double sqrt_s) const
 The ratio \(\mu_{WH,ZZ}\) between the WH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual double muWHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{WH,ZZ\to 4l}\) between the WH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual double muZH (const double sqrt_s) const
 The ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model. More...
 
virtual double muZHbb (const double sqrt_s) const
 The ratio \(\mu_{ZH,bb}\) between the ZH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual double muZHgaga (const double sqrt_s) const
 The ratio \(\mu_{ZH,\gamma\gamma}\) between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual double muZHmumu (const double sqrt_s) const
 The ratio \(\mu_{ZH,\mu\mu}\) between the ZH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual double muZHtautau (const double sqrt_s) const
 The ratio \(\mu_{ZH,\tau\tau}\) between the ZH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual double muZHWW (const double sqrt_s) const
 The ratio \(\mu_{ZH,WW}\) between the ZH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual double muZHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{ZH,WW\to 2l2\nu}\) between the ZH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual double muZHZga (const double sqrt_s) const
 The ratio \(\mu_{ZH,Z\gamma}\) between the ZH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual double muZHZZ (const double sqrt_s) const
 The ratio \(\mu_{ZH,ZZ}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual double muZHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{ZH,ZZ\to 4l}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual double Mw () const
 The mass of the \(W\) boson, \(M_W\). More...
 
 NPSMEFTd6 (const bool FlagLeptonUniversal_in=false, const bool FlagQuarkUniversal_in=false)
 Constructor. More...
 
virtual double obliqueS () const
 The oblique parameter \(S\). (Simplified implementation. Contribution only from \(O_{HWB}\).) More...
 
virtual double obliqueT () const
 The oblique parameter \(T\). (Simplified implementation. Contribution only from \(O_{HD}\).) More...
 
virtual double obliqueU () const
 The oblique parameter \(U\). More...
 
virtual double obliqueW () const
 The oblique parameter \(W\). (Simplified implementation. Contribution only from \(O_{2W}\).) More...
 
virtual double obliqueY () const
 The oblique parameter \(Y\). (Simplified implementation. Contribution only from \(O_{2B}\).) More...
 
virtual bool PostUpdate ()
 The post-update method for NPSMEFTd6. More...
 
virtual double ppZHprobe (const double sqrt_s) const
 The direction constrained by \( p p \to Z H\) in the boosted regime, \(g_p^Z\). From arXiv:1807.01796 and the contribution to FCC CDR Vol 1. Implemented only in NPSMEFTd6 class. More...
 
virtual bool setFlag (const std::string name, const bool value)
 A method to set a flag of NPSMEFTd6. More...
 
virtual double STXS_ggH0j (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual double STXS_ggH1j_pTH_0_60 (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual double STXS_ggH1j_pTH_120_200 (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual double STXS_ggH1j_pTH_200 (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual double STXS_ggH1j_pTH_60_120 (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual double STXS_ggH2j_pTH_0_200 (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual double STXS_ggH2j_pTH_0_60 (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual double STXS_ggH2j_pTH_120_200 (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual double STXS_ggH2j_pTH_200 (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual double STXS_ggH2j_pTH_60_120 (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual double STXS_ggH_VBFtopo_j3 (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual double STXS_ggH_VBFtopo_j3v (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual double STXS_qqHll_pTV_0_150 (const double sqrt_s) const
 The STXS bin \(qq \to H \ell \ell\). More...
 
virtual double STXS_qqHll_pTV_150_250 (const double sqrt_s) const
 The STXS bin \(qq \to H \ell \ell\). More...
 
virtual double STXS_qqHll_pTV_150_250_0j (const double sqrt_s) const
 The STXS bin \(qq \to H \ell \ell\). More...
 
virtual double STXS_qqHll_pTV_150_250_1j (const double sqrt_s) const
 The STXS bin \(qq \to H \ell \ell\). More...
 
virtual double STXS_qqHll_pTV_250 (const double sqrt_s) const
 The STXS bin \(qq \to H \ell \ell\). More...
 
virtual double STXS_qqHlv_pTV_0_150 (const double sqrt_s) const
 The STXS bin \(qq \to H \ell \nu\). More...
 
virtual double STXS_qqHlv_pTV_0_250 (const double sqrt_s) const
 The STXS bin \(qq \to H \ell \nu\). More...
 
virtual double STXS_qqHlv_pTV_150_250_0j (const double sqrt_s) const
 The STXS bin \(qq \to H \ell \nu\). More...
 
virtual double STXS_qqHlv_pTV_150_250_1j (const double sqrt_s) const
 The STXS bin \(qq \to H \ell \nu\). More...
 
virtual double STXS_qqHlv_pTV_250 (const double sqrt_s) const
 The STXS bin \(qq \to H \ell \nu\). More...
 
virtual double STXS_qqHqq_pTj_200 (const double sqrt_s) const
 The STXS bin \(qq \to H qq\). More...
 
virtual double STXS_qqHqq_Rest (const double sqrt_s) const
 The STXS bin \(qq \to H qq\). More...
 
virtual double STXS_qqHqq_VBFtopo_j3 (const double sqrt_s) const
 The STXS bin \(qq \to H qq\). More...
 
virtual double STXS_qqHqq_VBFtopo_j3v (const double sqrt_s) const
 The STXS bin \(qq \to H qq\). More...
 
virtual double STXS_qqHqq_VBFtopo_Rest (const double sqrt_s) const
 The STXS bin \(qq \to H qq\). More...
 
virtual double STXS_qqHqq_VHtopo (const double sqrt_s) const
 The STXS bin \(qq \to H qq\). More...
 
virtual double STXS_ttHtH (const double sqrt_s) const
 The STXS bin \( ttH + tH \). More...
 
virtual double STXS_WHqqHqq_pTj1_200 (const double sqrt_s) const
 The STXS bin \( qq \to WH \to H qq \). More...
 
virtual double STXS_WHqqHqq_Rest (const double sqrt_s) const
 The STXS bin \( qq \to WH \to H qq \). More...
 
virtual double STXS_WHqqHqq_VBFtopo_j3 (const double sqrt_s) const
 The STXS bin \( qq \to WH \to H qq \). More...
 
virtual double STXS_WHqqHqq_VBFtopo_j3v (const double sqrt_s) const
 The STXS bin \( qq \to WH \to H qq \). More...
 
virtual double STXS_WHqqHqq_VH2j (const double sqrt_s) const
 The STXS bin \( qq \to WH \to H qq \). More...
 
virtual double STXS_ZHqqHqq_pTj1_200 (const double sqrt_s) const
 The STXS bin \( qq \to ZH \to H qq \). More...
 
virtual double STXS_ZHqqHqq_Rest (const double sqrt_s) const
 The STXS bin \( qq \to ZH \to H qq \). More...
 
virtual double STXS_ZHqqHqq_VBFtopo_j3 (const double sqrt_s) const
 The STXS bin \( qq \to ZH \to H qq \). More...
 
virtual double STXS_ZHqqHqq_VBFtopo_j3v (const double sqrt_s) const
 The STXS bin \( qq \to ZH \to H qq \). More...
 
virtual double STXS_ZHqqHqq_VH2j (const double sqrt_s) const
 The STXS bin \( qq \to ZH \to H qq \). More...
 
virtual double xseeWW (const double sqrt_s) const
 Total \(e^+ e^- \to W^+ W^- \to jj \ell \nu\) cross section in pb, with \(\ell= e, \mu\). More...
 
- Public Member Functions inherited from NPbase
virtual double A_f (const Particle f) const
 The left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\mathcal{A}_f\). More...
 
virtual double AFB (const Particle f) const
 The forward-backward asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(A^f_{FB}\). More...
 
virtual double BR_Zf (const Particle f) const
 The Branching ratio of the \(Z\) boson into a given fermion pair, \(BR_Z^{f}\). More...
 
virtual double cbminuscc () const
 
virtual double cbminusctau () const
 
virtual double ccminusctau () const
 
virtual double cgaplusct () const
 
virtual double cgminuscga () const
 
virtual double cgplusct () const
 
virtual double cVpluscb () const
 
virtual double cVplusctau () const
 
virtual double deltaA_f (const Particle f) const
 The new physics contribution to the left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\delta \mathcal{A}_f\). More...
 
virtual double deltaAFB (const Particle f) const
 The new physics contribution to the forward-backward asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\delta A^f_{FB}\). More...
 
virtual double deltaGamma_Z () const
 The new physics contribution to the total decay width of the \(Z\) boson, \(\delta \Gamma_Z\). More...
 
virtual double deltaGamma_Zf (const Particle f) const
 The new physics contribution to the decay width of the \(Z\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\). More...
 
virtual double deltaGamma_Zhad () const
 The new physics contribution to the hadronic decay width of the \(Z\) boson, \(\delta \Gamma_{Z,had}\). More...
 
virtual double deltaN_nu () const
 The new physics contribution to the number of neutrinos dervied from the \(Z\) pole measurements. More...
 
virtual double deltaR0_f (const Particle f) const
 The new physics contribution to the ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\), \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\) and \(R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}\), for charged leptons, quarks and neutrinos, respectively. More...
 
virtual double deltaR_inv () const
 The new physics contribution to the ratio of invisible and leptonic (electron) decay widths of the \(Z\) boson, \(\delta R_{inv}\). More...
 
virtual double deltaSigmaHadron () const
 The new physics contribution to the cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\delta \sigma_h^0\). More...
 
virtual double deltaSin2thetaEff_e () const
 The new physics contribution to the effective electron/leptonic weak angle \(\delta \sin^2\theta_{\rm eff}^{\rm lept}\) at the \(Z\) pole. More...
 
virtual double deltaSin2thetaEff_mu () const
 The new physics contribution to the effective muonic weak angle \(\delta \sin^2\theta_{\rm eff}^{\mu\mu}\) at the \(Z\) pole. More...
 
virtual gslpp::complex gA_f (const Particle f) const
 The total (SM+NP) contribution to the neutral-current axial-vector coupling \(g_A^f\). More...
 
virtual double Gamma_had () const
 The hadronic decay width of the \(Z\) boson, \(\Gamma_{Z,had}\). More...
 
virtual double Gamma_Z () const
 The total decay width of the \(Z\) boson, \(\Gamma_Z\). More...
 
virtual double Gamma_Zf (const Particle f) const
 The decay width of the \(Z\) boson into a given fermion pair, \(\Gamma_Z^{f}\). More...
 
virtual StandardModel getTrueSM () const
 A method to return a StandardModel object from NPbase. More...
 
virtual gslpp::complex gV_f (const Particle f) const
 The total (SM+NP) contribution to the neutral-current vector coupling \(g_V^f\). More...
 
virtual gslpp::complex kappaZ_f (const Particle f) const
 The effective neutral-current coupling \(\kappa_Z^f\) including SM plus NP contributions. More...
 
virtual double muggHgagaInt (const double sqrt_s) const
 The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. Includes interference effects with the background, following arXiv:1704.08259. More...
 
virtual double muppHmumu (const double sqrt_s) const
 
virtual double muppHZga (const double sqrt_s) const
 
virtual double N_nu () const
 The number of neutrinos dervied from the \(Z\) pole measurements, \(N_{\nu}\). More...
 
 NPbase ()
 The default constructor. More...
 
virtual double R0_f (const Particle f) const
 The ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\), \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\) and \(R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}\), for charged leptons, quarks and neutrinos, respectively. More...
 
virtual double R_inv () const
 The ratio of the invisible and leptonic (electron) decay widths of the \(Z\) boson, \(R_{inv}\). More...
 
virtual gslpp::complex rhoZ_f (const Particle f) const
 The effective neutral-current coupling \(\rho_Z^f\) including SM plus NP contributions. More...
 
virtual double sigma0_had () const
 The cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\sigma_h^0\). More...
 
virtual double sin2thetaEff (const Particle f) const
 The leptonic effective weak mixing angle \(\sin^2\theta_{\rm eff}^{\rm lept}\) at the the \(Z\) pole. More...
 
virtual bool Update (const std::map< std::string, double > &DPars)
 The update method for NPbase. More...
 
virtual double UpperLimitZgammaA (const double sqrt_s) const
 
virtual double UpperLimitZgammaA13 (const double sqrt_s) const
 
virtual double UpperLimitZgammaC (const double sqrt_s) const
 
virtual double UpperLimitZgammaC13 (const double sqrt_s) const
 
- Public Member Functions inherited from StandardModel
double Ale (double mu, orders order, bool Nf_thr=true) const
 The running electromagnetic coupling \(\alpha_e(\mu)\) in the \(\overline{MS}\) scheme. More...
 
double ale_OS (const double mu, orders order=FULLNLO) const
 The running electromagnetic coupling \(\alpha(\mu)\) in the on-shell scheme. More...
 
double alphaMz () const
 The electromagnetic coupling at the \(Z\)-mass scale, \(\alpha(M_Z^2)=\alpha/(1-\Delta\alpha(M_Z^2))\). More...
 
double Als (double mu, orders order=FULLNLO, bool qed_flag=false, bool Nf_thr=true) const
 The running QCD coupling \(\alpha(\mu)\) in the \(\overline{MS}\) scheme including QED corrections. More...
 
double AlsByOrder (double mu, orders order=FULLNLO, bool qed_flag=false, bool Nf_thr=true) const
 
double Alstilde5 (const double mu) const
 The value of \(\frac{\alpha_s^{\mathrm{FULLNLO}}}{4\pi}\) at any scale \(\mu\) with the number of flavours \(n_f = 4\) and full EW corrections. More...
 
double Beta_e (int nm, unsigned int nf) const
 QED beta function coefficients - eq. (36) hep-ph/0512066. More...
 
double Beta_s (int nm, unsigned int nf) const
 QCD beta function coefficients including QED corrections - eq. (36) hep-ph/0512066. More...
 
double c02 () const
 The square of the cosine of the weak mixing angle \(c_0^2\) defined without weak radiative corrections. More...
 
virtual bool CheckFlags () const
 A method to check the sanity of the set of model flags. More...
 
bool checkSMparamsForEWPO ()
 A method to check whether the parameters relevant to the EWPO are updated. More...
 
double computeBrHtobb () const
 The Br \((H\to bb)\) in the Standard Model. More...
 
double computeBrHtocc () const
 The Br \((H\to cc)\) in the Standard Model. More...
 
double computeBrHtogaga () const
 The Br \((H\to\gamma\gamma)\) in the Standard Model. More...
 
double computeBrHtogg () const
 The Br \((H\to gg)\) in the Standard Model. More...
 
double computeBrHtomumu () const
 The Br \((H\to \mu\mu)\) in the Standard Model. More...
 
double computeBrHtoss () const
 The Br \((H\to ss)\) in the Standard Model. More...
 
double computeBrHtotautau () const
 The Br \((H\to \tau\tau)\) in the Standard Model. More...
 
double computeBrHtoWW () const
 The Br \((H\to WW)\) in the Standard Model. More...
 
double computeBrHtoZga () const
 The Br \((H\to Z\gamma)\) in the Standard Model. More...
 
double computeBrHtoZZ () const
 The Br \((H\to ZZ)\) in the Standard Model. More...
 
double computeBrHtoZZinv () const
 The Br \((H\to ZZ \to inv)\) in the Standard Model. More...
 
void ComputeDeltaR_rem (const double Mw_i, double DeltaR_rem[orders_EW_size]) const
 A method to collect \(\Delta r_{\mathrm{rem}}\) computed via subclasses. More...
 
void ComputeDeltaRho (const double Mw_i, double DeltaRho[orders_EW_size]) const
 A method to collect \(\Delta\rho\) computed via subclasses. More...
 
double computeGammaHgaga_tt () const
 The top loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More...
 
double computeGammaHgaga_tW () const
 The mixed \(t-W\) loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More...
 
double computeGammaHgaga_WW () const
 The \(W\) loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More...
 
double computeGammaHgg_bb () const
 The bottom loop contribution to \(H\to gg\) in the Standard Model. More...
 
double computeGammaHgg_tb () const
 The top-bottom interference contribution to \(H\to gg\) in the Standard Model. More...
 
double computeGammaHgg_tt () const
 The top loop contribution to \(H\to gg\) in the Standard Model. More...
 
double computeGammaHTotal () const
 The Higgs total width in the Standard Model. More...
 
double computeGammaHZga_tt () const
 The top loop contribution to \(H\to Z\gamma\) in the Standard Model. More...
 
double computeGammaHZga_tW () const
 The mixed \(t-W\) loop contribution to \(H\to Z\gamma\) in the Standard Model. More...
 
double computeGammaHZga_WW () const
 The \(W\) loop contribution to \(H\to Z\gamma\) in the Standard Model. Currently it returns the value of tab 41 in ref. [137]. More...
 
double computeSigmaggH (const double sqrt_s) const
 The ggH cross section in the Standard Model. More...
 
double computeSigmaggH_bb (const double sqrt_s) const
 The square of the bottom-quark contribution to the ggH cross section in the Standard Model. More...
 
double computeSigmaggH_tb (const double sqrt_s) const
 The top-bottom interference contribution to the ggH cross section in the Standard Model. More...
 
double computeSigmaggH_tt (const double sqrt_s) const
 The square of the top-quark contribution to the ggH cross section in the Standard Model. More...
 
double computeSigmattH (const double sqrt_s) const
 The ttH production cross section in the Standard Model. More...
 
double computeSigmaVBF (const double sqrt_s) const
 The VBF cross section in the Standard Model. More...
 
double computeSigmaWF (const double sqrt_s) const
 The W fusion contribution \(\sigma_{WF}\) to higgs-production cross section in the Standard Model. More...
 
double computeSigmaWH (const double sqrt_s) const
 The WH production cross section in the Standard Model. More...
 
double computeSigmaZF (const double sqrt_s) const
 The Z fusion contribution \(\sigma_{ZF}\) to higgs-production cross section in the Standard Model. More...
 
double computeSigmaZH (const double sqrt_s) const
 The ZH production cross section in the Standard Model. More...
 
double computeSigmaZWF (const double sqrt_s) const
 The Z W interference fusion contribution \(\sigma_{ZWF}\) to higgs-production cross section in the Standard Model. More...
 
virtual double cW2 () const
 
virtual double cW2 (const double Mw_i) const
 The square of the cosine of the weak mixing angle in the on-shell scheme, denoted as \(c_W^2\). More...
 
double DeltaAlpha () const
 The total corrections to the electromagnetic coupling \(\alpha\) at the \(Z\)-mass scale, denoted as \(\Delta\alpha(M_Z^2)\). More...
 
double DeltaAlphaL5q () const
 The sum of the leptonic and the five-flavour hadronic corrections to the electromagnetic coupling \(\alpha\) at the \(Z\)-mass scale, denoted as \(\Delta\alpha^{\ell+5q}(M_Z^2)\). More...
 
double DeltaAlphaLepton (const double s) const
 Leptonic contribution to the electromagnetic coupling \(\alpha\), denoted as \(\Delta\alpha_{\mathrm{lept}}(s)\). More...
 
double DeltaAlphaTop (const double s) const
 Top-quark contribution to the electromagnetic coupling \(\alpha\), denoted as \(\Delta\alpha_{\mathrm{top}}(s)\). More...
 
virtual gslpp::complex deltaKappaZ_f (const Particle f) const
 Flavour non-universal vertex corrections to \(\kappa_Z^l\), denoted by \(\Delta\kappa_Z^l\). More...
 
virtual double DeltaR () const
 The SM prediction for \(\Delta r\) derived from that for the \(W\) boson mass. More...
 
virtual double DeltaRbar () const
 The SM prediction for \(\Delta \overline{r}\) derived from that for the \(W\)-boson mass. More...
 
virtual gslpp::complex deltaRhoZ_f (const Particle f) const
 Flavour non-universal vertex corrections to \(\rho_Z^l\), denoted by \(\Delta\rho_Z^l\). More...
 
virtual double epsilon1 () const
 The SM contribution to the epsilon parameter \(\varepsilon_1\). More...
 
virtual double epsilon2 () const
 The SM contribution to the epsilon parameter \(\varepsilon_2\). More...
 
virtual double epsilon3 () const
 The SM contribution to the epsilon parameter \(\varepsilon_3\). More...
 
virtual double epsilonb () const
 The SM contribution to the epsilon parameter \(\varepsilon_b\). More...
 
virtual double Gamma_inv () const
 The invisible partial decay width of the \(Z\) boson, \(\Gamma_{\mathrm{inv}}\). More...
 
virtual double GammaZ (const Particle f) const
 The \(Z\to \ell\bar{\ell}\) partial decay width, \(\Gamma_\ell\). More...
 
double getAle () const
 A get method to retrieve the fine-structure constant \(\alpha\). More...
 
double getAlsMz () const
 A get method to access the value of \(\alpha_s(M_Z)\). More...
 
virtual double getCBd () const
 The ratio of the absolute value of the $B_d$ mixing amplitude over the Standard Model value. More...
 
virtual double getCBs () const
 The ratio of the absolute value of the $B_s$ mixing amplitude over the Standard Model value. More...
 
virtual double getCCC1 () const
 A virtual implementation for the RealWeakEFTCC class. More...
 
virtual double getCCC2 () const
 A virtual implementation for the RealWeakEFTCC class. More...
 
virtual double getCCC3 () const
 A virtual implementation for the RealWeakEFTCC class. More...
 
virtual double getCCC4 () const
 A virtual implementation for the RealWeakEFTCC class. More...
 
virtual double getCCC5 () const
 A virtual implementation for the RealWeakEFTCC class. More...
 
virtual double getCDMK () const
 The ratio of the real part of the $K$ mixing amplitude over the Standard Model value. More...
 
virtual double getCepsK () const
 The ratio of the imaginary part of the $K$ mixing amplitude over the Standard Model value. More...
 
CKM getCKM () const
 A get method to retrieve the member object of type CKM. More...
 
double getDAle5Mz () const
 A get method to retrieve the five-flavour hadronic contribution to the electromagnetic coupling, \(\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)\). More...
 
double getDelGammaZ () const
 A get method to retrieve the theoretical uncertainty in \(\Gamma_Z\), denoted as \(\delta\,\Gamma_Z\). More...
 
double getDelMw () const
 A get method to retrieve the theoretical uncertainty in \(M_W\), denoted as \(\delta\,M_W\). More...
 
double getDelR0b () const
 A get method to retrieve the theoretical uncertainty in \(R_b^0\), denoted as \(\delta\,R_b^0\). More...
 
double getDelR0c () const
 A get method to retrieve the theoretical uncertainty in \(R_c^0\), denoted as \(\delta\,R_c^0\). More...
 
double getDelR0l () const
 A get method to retrieve the theoretical uncertainty in \(R_l^0\), denoted as \(\delta\,R_l^0\). More...
 
double getDelSigma0H () const
 A get method to retrieve the theoretical uncertainty in \(\sigma_{Hadron}^0\), denoted as \(\delta\,\sigma_{Hadron}^0\). More...
 
double getDelSin2th_b () const
 A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{b}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{b}\). More...
 
double getDelSin2th_l () const
 A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{\rm lept}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{\rm lept}\). More...
 
double getDelSin2th_q () const
 A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{q\not = b,t}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{q\not = b,t}\). More...
 
std::string getFlagKappaZ () const
 A method to retrieve the model flag KappaZ. More...
 
std::string getFlagMw () const
 A method to retrieve the model flag Mw. More...
 
std::string getFlagRhoZ () const
 A method to retrieve the model flag RhoZ. More...
 
const FlavourgetFlavour () const
 
double getGF () const
 A get method to retrieve the Fermi constant \(G_\mu\). More...
 
int getIterationNo () const
 
Particle getLeptons (const QCD::lepton p) const
 A get method to retrieve the member object of a lepton. More...
 
virtual double getMHl () const
 A get method to retrieve the Higgs mass \(m_h\). More...
 
virtual double getmq (const QCD::quark q, const double mu) const
 
double getMuw () const
 A get method to retrieve the matching scale \(\mu_W\) around the weak scale. More...
 
EWSMApproximateFormulaegetMyApproximateFormulae () const
 A get method to retrieve the member pointer of type EWSMApproximateFormulae. More...
 
EWSMcachegetMyEWSMcache () const
 A get method to retrieve the member pointer of type EWSMcache. More...
 
LeptonFlavourgetMyLeptonFlavour () const
 
EWSMOneLoopEWgetMyOneLoopEW () const
 A get method to retrieve the member pointer of type EWSMOneLoopEW,. More...
 
EWSMThreeLoopEWgetMyThreeLoopEW () const
 
EWSMThreeLoopEW2QCDgetMyThreeLoopEW2QCD () const
 
EWSMThreeLoopQCDgetMyThreeLoopQCD () const
 
EWSMTwoLoopEWgetMyTwoLoopEW () const
 
EWSMTwoLoopQCDgetMyTwoLoopQCD () const
 
double getMz () const
 A get method to access the mass of the \(Z\) boson \(M_Z\). More...
 
virtual double getPhiBd () const
 Half the relative phase of the $B_d$ mixing amplitude w.r.t. the Standard Model one. More...
 
virtual double getPhiBs () const
 Half the relative phase of the $B_s$ mixing amplitude w.r.t. the Standard Model one. More...
 
gslpp::matrix< gslpp::complexgetUPMNS () const
 A get method to retrieve the object of the PMNS matrix. More...
 
gslpp::matrix< gslpp::complexgetVCKM () const
 A get method to retrieve the CKM matrix. More...
 
gslpp::matrix< gslpp::complexgetYd () const
 A get method to retrieve the Yukawa matrix of the down-type quarks, \(Y_d\). More...
 
gslpp::matrix< gslpp::complexgetYe () const
 A get method to retrieve the Yukawa matrix of the charged leptons, \(Y_e\). More...
 
gslpp::matrix< gslpp::complexgetYn () const
 A get method to retrieve the Yukawa matrix of the neutrinos, \(Y_\nu\). More...
 
gslpp::matrix< gslpp::complexgetYu () const
 A get method to retrieve the Yukawa matrix of the up-type quarks, \(Y_u\). More...
 
virtual bool Init (const std::map< std::string, double > &DPars)
 A method to initialize the model parameters. More...
 
virtual bool InitializeModel ()
 A method to initialize the model. More...
 
bool IsFlagNoApproximateGammaZ () const
 A method to retrieve the model flag NoApproximateGammaZ. More...
 
bool IsFlagWithoutNonUniversalVC () const
 A method to retrieve the model flag WithoutNonUniversalVC. More...
 
virtual double Mw_tree () const
 The tree-level mass of the \(W\) boson, \(M_W^{\mathrm{tree}}\). More...
 
double MwbarFromMw (const double Mw) const
 A method to convert the \(W\)-boson mass in the experimental/running-width scheme to that in the complex-pole/fixed-width scheme. More...
 
double MwFromMwbar (const double Mwbar) const
 A method to convert the \(W\)-boson mass in the complex-pole/fixed-width scheme to that in the experimental/running-width scheme. More...
 
double Mzbar () const
 The \(Z\)-boson mass \(\overline{M}_Z\) in the complex-pole/fixed-width scheme. More...
 
virtual bool PreUpdate ()
 The pre-update method for StandardModel. More...
 
virtual double rho_GammaW (const Particle fi, const Particle fj) const
 EW radiative corrections to the width of \(W \to f_i \bar{f}_j\), denoted as \(\rho^W_{ij}\). More...
 
double s02 () const
 The square of the sine of the weak mixing angle \(s_0^2\) defined without weak radiative corrections. More...
 
void setFlagCacheInStandardModel (bool FlagCacheInStandardModel)
 A set method to change the model flag CacheInStandardModel of StandardModel. More...
 
void setFlagNoApproximateGammaZ (bool FlagNoApproximateGammaZ)
 
virtual bool setFlagStr (const std::string name, const std::string value)
 A method to set a flag of StandardModel. More...
 
 StandardModel ()
 The default constructor. More...
 
double sW2 () const
 
virtual double sW2 (const double Mw_i) const
 The square of the sine of the weak mixing angle in the on-shell scheme, denoted as \(s_W^2\). More...
 
virtual double v () const
 The Higgs vacuum expectation value. More...
 
virtual ~StandardModel ()
 The default destructor. More...
 
- Public Member Functions inherited from QCD
double AboveTh (const double mu) const
 The active flavour threshold above the scale \(\mu\) as defined in QCD::Thresholds(). More...
 
void addParameters (std::vector< std::string > params_i)
 A method to add parameters that are specific to only one set of observables. More...
 
virtual double Als (const double mu, const orders order=FULLNLO, bool Nf_thr=true) const
 
double Als4 (const double mu) const
 The value of \(\alpha_s^{\mathrm{FULLNLO}}\) at any scale \(\mu\) with the number of flavours \(n_f = 4\). More...
 
virtual double AlsByOrder (const double mu, const orders order=FULLNLO, bool Nf_thr=true) const
 
double AlsOLD (const double mu, const orders order=FULLNLO) const
 Computes the running strong coupling \(\alpha_s(\mu)\) in the \(\overline{\mathrm{MS}}\) scheme. In the cases of LO, NLO and FULLNNLO, the coupling is computed with AlsWithInit(). On the other hand, in the cases of NNLO and FULLNNLO, the coupling is computed with AlsWithLambda(). More...
 
double AlsWithInit (const double mu, const double alsi, const double mu_i, const orders order) const
 Computes the running strong coupling \(\alpha_s(\mu)\) from \(\alpha_s(\mu_i)\) in the \(\overline{\mathrm{MS}}\) scheme, where it is forbidden to across a flavour threshold in the RG running from \(\mu_i\) to \(\mu\). More...
 
double AlsWithLambda (const double mu, const orders order) const
 Computes the running strong coupling \(\alpha_s(\mu)\) in the \(\overline{\mathrm{MS}}\) scheme with the use of \(\Lambda_{\rm QCD}\). More...
 
double BelowTh (const double mu) const
 The active flavour threshold below the scale \(\mu\) as defined in QCD::Thresholds(). More...
 
double Beta0 (const double nf) const
 The \(\beta_0(n_f)\) coefficient for a certain number of flavours \(n_f\). More...
 
double Beta1 (const double nf) const
 The \(\beta_1(n_f)\) coefficient for a certain number of flavours \(n_f\). More...
 
double Beta2 (const double nf) const
 The \(\beta_2(n_f)\) coefficient for a certain number of flavours \(n_f\). More...
 
double Beta3 (const double nf) const
 The \(\beta_3(n_f)\) coefficient for a certain number of flavours \(n_f\). More...
 
void CacheShift (double cache[][5], int n) const
 A member used to manage the caching for this class. More...
 
void CacheShift (int cache[][5], int n) const
 
orders FullOrder (orders order) const
 Return the FULLORDER enum corresponding to order. More...
 
double Gamma0 (const double nf) const
 The \(\gamma_0\) coefficient used to compute the running of a mass. More...
 
double Gamma1 (const double nf) const
 The \(\gamma_1\) coefficient used to compute the running of a mass. More...
 
double Gamma2 (const double nf) const
 The \(\gamma_2\) coefficient used to compute the running of a mass. More...
 
double getAlsM () const
 A get method to access the value of \(\alpha_s(M_{\alpha_s})\). More...
 
BParameter getBBd () const
 For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta b = 2\) process in the \(B_d\) meson system. More...
 
BParameter getBBs () const
 For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta b = 2\) process in the \(B_s\) meson system. More...
 
BParameter getBD () const
 For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta c = 2\) process in the \(D^0\) meson system. More...
 
BParameter getBK () const
 For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta s = 2\) process in the \(K^0\) meson system. More...
 
BParameter getBKd1 () const
 
BParameter getBKd3 () const
 
double getCF () const
 A get method to access the Casimir factor of QCD. More...
 
double getMAls () const
 A get method to access the mass scale \(M_{\alpha_s}\) at which the strong coupling constant measurement is provided. More...
 
Meson getMesons (const QCD::meson m) const
 A get method to access a meson as an object of the type Meson. More...
 
double getMtpole () const
 A get method to access the pole mass of the top quark. More...
 
double getMub () const
 A get method to access the threshold between five- and four-flavour theory in GeV. More...
 
double getMuc () const
 A get method to access the threshold between four- and three-flavour theory in GeV. More...
 
double getMut () const
 A get method to access the threshold between six- and five-flavour theory in GeV. More...
 
double getNc () const
 A get method to access the number of colours \(N_c\). More...
 
double getOptionalParameter (std::string name) const
 A method to get parameters that are specific to only one set of observables. More...
 
Particle getQuarks (const QCD::quark q) const
 A get method to access a quark as an object of the type Particle. More...
 
std::vector< std::string > getUnknownParameters ()
 A method to get the vector of the parameters that have been specified in the configuration file but not being used. More...
 
void initializeBParameter (std::string name_i) const
 A method to initialize B Parameter and the corresponding meson. More...
 
void initializeMeson (QCD::meson meson_i) const
 A method to initialize a meson. More...
 
double logLambda (const double nf, orders order) const
 Computes \(\ln\Lambda_\mathrm{QCD}\) with nf flavours in GeV. More...
 
double Mbar2Mp (const double mbar, const orders order=FULLNNLO) const
 Converts the \(\overline{\mathrm{MS}}\) mass \(m(m)\) to the pole mass. More...
 
double Mp2Mbar (const double mp, const orders order=FULLNNLO) const
 Converts a quark pole mass to the corresponding \(\overline{\mathrm{MS}}\) mass \(m(m)\). More...
 
double Mrun (const double mu, const double m, const orders order=FULLNNLO) const
 Computes a running quark mass \(m(\mu)\) from \(m(m)\). More...
 
double Mrun (const double mu_f, const double mu_i, const double m, const orders order=FULLNNLO) const
 Runs a quark mass from \(\mu_i\) to \(\mu_f\). More...
 
double Mrun4 (const double mu_f, const double mu_i, const double m) const
 The running of a mass with the number of flavours \(n_f = 4\). More...
 
double MS2DRqmass (const double MSbar) const
 Converts a quark mass from the \(\overline{\mathrm{MS}}\) scheme to the \(\overline{\mathrm{DR}}\) scheme. More...
 
double MS2DRqmass (const double MSscale, const double MSbar) const
 Converts a quark mass from the \(\overline{\mathrm{MS}}\) scheme to the \(\overline{\mathrm{DR}}\) scheme. More...
 
double Nf (const double mu) const
 The number of active flavour at scale \(\mu\). More...
 
double NfThresholdCorrections (double mu, double M, double als, int nf, orders order) const
 Threshold corrections in matching \(\alpha_s(n_f+1)\) with \(\alpha_s(n_f)\) from eq. (34) of hep-ph/0512060. More...
 
std::string orderToString (const orders order) const
 Converts an object of the enum type "orders" to the corresponding string. More...
 
 QCD ()
 Constructor. More...
 
void setNc (double Nc)
 A set method to change the number of colours \(N_c\). More...
 
void setOptionalParameter (std::string name, double value)
 A method to set the parameter value for the parameters that are specific to only one set of observables. More...
 
double Thresholds (const int i) const
 For accessing the active flavour threshold scales. More...
 
- Public Member Functions inherited from Model
void addMissingModelParameter (const std::string &missingParameterName)
 
std::vector< std::string > getmissingModelParameters ()
 
unsigned int getMissingModelParametersCount ()
 
std::string getModelName () const
 A method to fetch the name of the model. More...
 
const double & getModelParam (std::string name) const
 
bool isModelGeneralTHDM () const
 
bool isModelGeorgiMachacek () const
 
bool IsModelInitialized () const
 A method to check if the model is initialized. More...
 
bool isModelLinearized () const
 
bool isModelParam (std::string name) const
 
bool isModelSUSY () const
 
bool isModelTHDM () const
 
bool isModelTHDMW () const
 
bool IsUpdateError () const
 A method to check if there was any error in the model update process. More...
 
 Model ()
 The default constructor. More...
 
void raiseMissingModelParameterCount ()
 
void setModelGeneralTHDM ()
 
void setModelGeorgiMachacek ()
 
void setModelInitialized (bool ModelInitialized)
 A set method to fix the failure or success of the initialization of the model. More...
 
void setModelLinearized (bool linearized=true)
 
void setModelName (const std::string name)
 A method to set the name of the model. More...
 
void setModelSUSY ()
 
void setModelTHDM ()
 
void setModelTHDMW ()
 
void setSliced (bool Sliced)
 
void setUpdateError (bool UpdateError)
 A set method to fix the update status as success or failure. More...
 
virtual ~Model ()
 The default destructor. More...
 

Static Public Attributes

static const int NNPSMEFTd6Vars = 446
 The number of the model parameters in NPSMEFTd6. More...
 
static const int NNPSMEFTd6Vars_LFU_QFU = 250
 The number of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities. More...
 
static const std::string NPSMEFTd6Vars [NNPSMEFTd6Vars]
 A string array containing the labels of the model parameters in NPSMEFTd6 if the model flag FlagRotateCHWCHB=false. More...
 
static const std::string NPSMEFTd6Vars_LFU_QFU [NNPSMEFTd6Vars_LFU_QFU]
 A string array containing the labels of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities if the model flag FlagRotateCHWCHB=false. More...
 
static const std::string NPSMEFTd6VarsRot [NNPSMEFTd6Vars]
 A string array containing the labels of the model parameters in NPSMEFTd6 if the model flag FlagRotateCHWCHB=true. More...
 
static const std::string NPSMEFTd6VarsRot_LFU_QFU [NNPSMEFTd6Vars_LFU_QFU]
 A string array containing the labels of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities if the model flag FlagRotateCHWCHB=true. More...
 
- Static Public Attributes inherited from StandardModel
static const double GeVminus2_to_nb = 389379.338
 
static const double Mw_error = 0.00001
 The target accuracy of the iterative calculation of the \(W\)-boson mass in units of GeV. More...
 
static const int NSMvars = 26
 The number of the model parameters in StandardModel. More...
 
static const int NumSMParamsForEWPO = 33
 The number of the SM parameters that are relevant to the EW precision observables. More...
 
static std::string SMvars [NSMvars]
 A string array containing the labels of the model parameters in StandardModel. More...
 
- Static Public Attributes inherited from QCD
static const int NQCDvars = 11
 The number of model parameters in QCD. More...
 
static std::string QCDvars [NQCDvars]
 An array containing the labels under which all QCD parameters are stored in a vector of ModelParameter via InputParser::ReadParameters(). More...
 

Protected Member Functions

gslpp::complex CfB_diag (const Particle f) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{EB,UB,DB}\) corresponding to particle f. More...
 
gslpp::complex CfG_diag (const Particle f) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{UG,DG}\) corresponding to particle f. More...
 
gslpp::complex CfH_diag (const Particle f) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{EH,UH,DH}\) corresponding to particle f. More...
 
gslpp::complex CfW_diag (const Particle f) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{EW,UW,DW}\) corresponding to particle f. More...
 
double CHF1_diag (const Particle F) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(1)}\) corresponding to particle F. More...
 
double CHF3_diag (const Particle F) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(3)}\) corresponding to particle F. More...
 
double CHf_diag (const Particle f) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{HE,HU,HD}\) corresponding to particle f. More...
 
gslpp::complex CHud_diag (const Particle u) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{Hud}\) corresponding to particle f. More...
 
virtual void setParameter (const std::string name, const double &value)
 A method to set the value of a parameter of the model. More...
 
- Protected Member Functions inherited from StandardModel
bool checkEWPOscheme (const std::string scheme) const
 A method to check if a given scheme name in string form is valid. More...
 
virtual void computeCKM ()
 The method to compute the CKM matrix. More...
 
virtual void computeYukawas ()
 The method to compute the Yukawa matrices. More...
 
double Delta_EWQCD (const QCD::quark q) const
 The non-factorizable EW-QCD corrections to the partial widths for \(Z\to q\bar{q}\), denoted as \(\Delta_{\mathrm{EW/QCD}}\). More...
 
double m_q (const QCD::quark q, const double mu, const orders order=FULLNLO) const
 
double RAq (const QCD::quark q) const
 The radiator factor associated with the final-state QED and QCD corrections to the the axial-vector-current interactions, \(R_A^q(M_Z^2)\). More...
 
double resumKappaZ (const double DeltaRho[orders_EW_size], const double deltaKappa_rem[orders_EW_size], const double DeltaRbar_rem, const bool bool_Zbb) const
 A method to compute the real part of the effetvive coupling \(\kappa_Z^f\) from \(\Delta\rho\), \(\delta\rho_{\rm rem}^{f}\) and \(\Delta r_{\mathrm{rem}}\). More...
 
double resumMw (const double Mw_i, const double DeltaRho[orders_EW_size], const double DeltaR_rem[orders_EW_size]) const
 A method to compute the \(W\)-boson mass from \(\Delta\rho\) and \(\Delta r_{\mathrm{rem}}\). More...
 
double resumRhoZ (const double DeltaRho[orders_EW_size], const double deltaRho_rem[orders_EW_size], const double DeltaRbar_rem, const bool bool_Zbb) const
 A method to compute the real part of the effective coupling \(\rho_Z^f\) from \(\Delta\rho\), \(\delta\rho_{\rm rem}^{f}\) and \(\Delta r_{\mathrm{rem}}\). More...
 
double RVh () const
 The singlet vector corrections to the hadronic \(Z\)-boson width, denoted as \(R_V^h\). More...
 
double RVq (const QCD::quark q) const
 The radiator factor associated with the final-state QED and QCD corrections to the the vector-current interactions, \(R_V^q(M_Z^2)\). More...
 
double SchemeToDouble (const std::string scheme) const
 A method to convert a given scheme name in string form into a floating-point number with double precision. More...
 
double taub () const
 Top-mass corrections to the \(Zb\bar{b}\) vertex, denoted by \(\tau_b\). More...
 
- Protected Member Functions inherited from QCD
double MassOfNf (int nf) const
 The Mbar mass of the heaviest quark in the theory with Nf active flavour. More...
 

Protected Attributes

double ai2G
 
double ai3G
 
double aiA
 
double aiB
 
double aiG
 
double aiH
 
double aiHB
 
double aiHd
 
double aiHe
 
double aiHL
 
double aiHQ
 
double aiHu
 
double aiHW
 
double aipHL
 
double aipHQ
 
double aiT
 
double aiu
 
double aiuG
 
double aiWW
 
double aleMz
 The em constant at Mz. More...
 
double BrHexo
 The branching ratio of exotic (not invisible) Higgs decays. More...
 
double BrHinv
 The branching ratio of invisible Higgs decays. More...
 
double C2B
 The dimension-6 operator coefficient \(C_{2W}\). More...
 
double C2BS
 The dimension-6 operator coefficient \(C_{2W}^{SILH}\). More...
 
double C2W
 The dimension-6 operator coefficient \(C_{2B}\). More...
 
double C2WS
 The dimension-6 operator coefficient \(C_{2B}^{SILH}\). More...
 
double CDB
 The dimension-6 operator coefficient \(C_{DB}\). More...
 
double CdH_11i
 The dimension-6 operator coefficient \((C_{dH})_{11}\) (imaginary part). More...
 
double CdH_11r
 The dimension-6 operator coefficient \((C_{dH})_{11}\) (real part). More...
 
double CdH_12i
 The dimension-6 operator coefficient \((C_{dH})_{12}\) (imaginary part). More...
 
double CdH_12r
 The dimension-6 operator coefficient \((C_{dH})_{12}\) (real part). More...
 
double CdH_13i
 The dimension-6 operator coefficient \((C_{dH})_{13}\) (imaginary part). More...
 
double CdH_13r
 The dimension-6 operator coefficient \((C_{dH})_{13}\) (real part). More...
 
double CdH_22i
 The dimension-6 operator coefficient \((C_{dH})_{22}\) (imaginary part). More...
 
double CdH_22r
 The dimension-6 operator coefficient \((C_{dH})_{22}\) (real part). More...
 
double CdH_23i
 The dimension-6 operator coefficient \((C_{dH})_{23}\) (imaginary part). More...
 
double CdH_23r
 The dimension-6 operator coefficient \((C_{dH})_{23}\) (real part). More...
 
double CdH_33i
 The dimension-6 operator coefficient \((C_{dH})_{33}\) (imaginary part). More...
 
double CdH_33r
 The dimension-6 operator coefficient \((C_{dH})_{33}\) (real part). More...
 
double CDHB
 The dimension-6 operator coefficient \(C_{DHB}\). More...
 
double CDHW
 The dimension-6 operator coefficient \(C_{DHW}\). More...
 
double CDW
 The dimension-6 operator coefficient \(C_{DW}\). More...
 
double Ced_1111
 
double Ced_1122
 
double Ced_1123
 
double Ced_1132
 
double Ced_1133
 
double Ced_2211
 
double Ced_2223
 
double Ced_2232
 
double Ced_3311
 
double Ced_3323
 
double Ced_3332
 
double Cee_1111
 
double Cee_1122
 
double Cee_1133
 
double Cee_2211
 
double Cee_3311
 
double CeH_11i
 The dimension-6 operator coefficient \((C_{eH})_{11}\) (imaginary part). More...
 
double CeH_11r
 The dimension-6 operator coefficient \((C_{eH})_{11}\) (real part). More...
 
double CeH_12i
 The dimension-6 operator coefficient \((C_{eH})_{12}\) (imaginary part). More...
 
double CeH_12r
 The dimension-6 operator coefficient \((C_{eH})_{12}\) (real part). More...
 
double CeH_13i
 The dimension-6 operator coefficient \((C_{eH})_{13}\) (imaginary part). More...
 
double CeH_13r
 The dimension-6 operator coefficient \((C_{eH})_{13}\) (real part). More...
 
double CeH_22i
 The dimension-6 operator coefficient \((C_{eH})_{22}\) (imaginary part). More...
 
double CeH_22r
 The dimension-6 operator coefficient \((C_{eH})_{22}\) (real part). More...
 
double CeH_23i
 The dimension-6 operator coefficient \((C_{eH})_{23}\) (imaginary part). More...
 
double CeH_23r
 The dimension-6 operator coefficient \((C_{eH})_{23}\) (real part). More...
 
double CeH_33i
 The dimension-6 operator coefficient \((C_{eH})_{33}\) (imaginary part). More...
 
double CeH_33r
 The dimension-6 operator coefficient \((C_{eH})_{33}\) (real part). More...
 
double Ceu_1111
 
double Ceu_1122
 
double Ceu_1133
 
double Ceu_2211
 
double Ceu_2233
 
double Ceu_3311
 
double CG
 The dimension-6 operator coefficient \(C_{G}\). More...
 
double CH
 The dimension-6 operator coefficient \(C_{H}\). More...
 
double CHB
 The dimension-6 operator coefficient \(C_{HB}\). More...
 
double CHbox
 The dimension-6 operator coefficient \(C_{H\Box}\). More...
 
double CHD
 The dimension-6 operator coefficient \(C_{HD}\). More...
 
double CHd_11
 The dimension-6 operator coefficient \((C_{Hd})_{11}\). More...
 
double CHd_12i
 The dimension-6 operator coefficient \((C_{Hd})_{12}\) (imaginary part). More...
 
double CHd_12r
 The dimension-6 operator coefficient \((C_{Hd})_{12}\) (real part). More...
 
double CHd_13i
 The dimension-6 operator coefficient \((C_{Hd})_{13}\) (imaginary part). More...
 
double CHd_13r
 The dimension-6 operator coefficient \((C_{Hd})_{13}\) (real part). More...
 
double CHd_22
 The dimension-6 operator coefficient \((C_{Hd})_{22}\). More...
 
double CHd_23i
 The dimension-6 operator coefficient \((C_{Hd})_{23}\) (imaginary part). More...
 
double CHd_23r
 The dimension-6 operator coefficient \((C_{Hd})_{23}\) (real part). More...
 
double CHd_33
 The dimension-6 operator coefficient \((C_{Hd})_{33}\). More...
 
double CHe_11
 The dimension-6 operator coefficient \((C_{He})_{11}\). More...
 
double CHe_12i
 The dimension-6 operator coefficient \((C_{He})_{12}\) (imaginary part). More...
 
double CHe_12r
 The dimension-6 operator coefficient \((C_{He})_{12}\) (real part). More...
 
double CHe_13i
 The dimension-6 operator coefficient \((C_{He})_{13}\) (imaginary part). More...
 
double CHe_13r
 The dimension-6 operator coefficient \((C_{He})_{13}\) (real part). More...
 
double CHe_22
 The dimension-6 operator coefficient \((C_{He})_{22}\). More...
 
double CHe_23i
 The dimension-6 operator coefficient \((C_{He})_{23}\) (imaginary part). More...
 
double CHe_23r
 The dimension-6 operator coefficient \((C_{He})_{23}\) (real part). More...
 
double CHe_33
 The dimension-6 operator coefficient \((C_{He})_{33}\). More...
 
double CHG
 The dimension-6 operator coefficient \(C_{HG}\). More...
 
double CHL1_11
 The dimension-6 operator coefficient \((C_{HL}^{(1)})_{11}\). More...
 
double CHL1_12i
 The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (imaginary part). More...
 
double CHL1_12r
 The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (real part). More...
 
double CHL1_13i
 The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (imaginary part). More...
 
double CHL1_13r
 The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (real part). More...
 
double CHL1_22
 The dimension-6 operator coefficient \((C_{HL}^{(1)})_{22}\). More...
 
double CHL1_23i
 The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (imaginary part). More...
 
double CHL1_23r
 The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (real part). More...
 
double CHL1_33
 The dimension-6 operator coefficient \((C_{HL}^{(1)})_{33}\). More...
 
double CHL3_11
 The dimension-6 operator coefficient \((C_{HL}^{(3)})_{11}\). More...
 
double CHL3_12i
 The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part). More...
 
double CHL3_12r
 The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part). More...
 
double CHL3_13i
 The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part). More...
 
double CHL3_13r
 The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part). More...
 
double CHL3_22
 The dimension-6 operator coefficient \((C_{HL}^{(3)})_{22}\). More...
 
double CHL3_23i
 The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part). More...
 
double CHL3_23r
 The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part). More...
 
double CHL3_33
 The dimension-6 operator coefficient \((C_{HL}^{(3)})_{33}\). More...
 
double CHQ1_11
 The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{11}\). More...
 
double CHQ1_12i
 The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (imaginary part). More...
 
double CHQ1_12r
 The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (real part). More...
 
double CHQ1_13i
 The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (imaginary part). More...
 
double CHQ1_13r
 The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (real part). More...
 
double CHQ1_22
 The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{22}\). More...
 
double CHQ1_23i
 The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (imaginary part). More...
 
double CHQ1_23r
 The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (real part). More...
 
double CHQ1_33
 The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{33}\). More...
 
double CHQ3_11
 The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{11}\). More...
 
double CHQ3_12i
 The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (imaginary part). More...
 
double CHQ3_12r
 The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (real part). More...
 
double CHQ3_13i
 The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (imaginary part). More...
 
double CHQ3_13r
 The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (real part). More...
 
double CHQ3_22
 The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{22}\). More...
 
double CHQ3_23i
 The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (imaginary part). More...
 
double CHQ3_23r
 The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (real part). More...
 
double CHQ3_33
 The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{33}\). More...
 
double cHSM
 Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes. More...
 
double CHu_11
 The dimension-6 operator coefficient \((C_{Hu})_{11}\). More...
 
double CHu_12i
 The dimension-6 operator coefficient \((C_{Hu})_{12}\) (imaginary part). More...
 
double CHu_12r
 The dimension-6 operator coefficient \((C_{Hu})_{12}\) (real part). More...
 
double CHu_13i
 The dimension-6 operator coefficient \((C_{Hu})_{13}\) (imaginary part). More...
 
double CHu_13r
 The dimension-6 operator coefficient \((C_{Hu})_{13}\) (real part). More...
 
double CHu_22
 The dimension-6 operator coefficient \((C_{Hu})_{22}\). More...
 
double CHu_23i
 The dimension-6 operator coefficient \((C_{Hu})_{23}\) (imaginary part). More...
 
double CHu_23r
 The dimension-6 operator coefficient \((C_{Hu})_{23}\) (real part). More...
 
double CHu_33
 The dimension-6 operator coefficient \((C_{Hu})_{33}\). More...
 
double CHud_11i
 The dimension-6 operator coefficient \((C_{Hud})_{11}\) (imaginary part). More...
 
double CHud_11r
 The dimension-6 operator coefficient \((C_{Hud})_{11}\) (real part). More...
 
double CHud_12i
 The dimension-6 operator coefficient \((C_{Hud})_{12}\) (imaginary part). More...
 
double CHud_12r
 The dimension-6 operator coefficient \((C_{Hud})_{12}\) (real part). More...
 
double CHud_13i
 The dimension-6 operator coefficient \((C_{Hud})_{13}\) (imaginary part). More...
 
double CHud_13r
 The dimension-6 operator coefficient \((C_{Hud})_{13}\) (real part). More...
 
double CHud_22i
 The dimension-6 operator coefficient \((C_{Hud})_{22}\) (imaginary part). More...
 
double CHud_22r
 The dimension-6 operator coefficient \((C_{Hud})_{22}\) (real part). More...
 
double CHud_23i
 The dimension-6 operator coefficient \((C_{Hud})_{23}\) (imaginary part). More...
 
double CHud_23r
 The dimension-6 operator coefficient \((C_{Hud})_{23}\) (real part). More...
 
double CHud_33i
 The dimension-6 operator coefficient \((C_{Hud})_{33}\) (imaginary part). More...
 
double CHud_33r
 The dimension-6 operator coefficient \((C_{Hud})_{33}\) (real part). More...
 
double CHW
 The dimension-6 operator coefficient \(C_{HW}\). More...
 
double CHWB
 The dimension-6 operator coefficient \(C_{HWB}\). More...
 
double CHWHB_gaga
 The combination of dimension-6 operator coefficients entering in \(\delta_{AA}\): \(s_W^2 C_{HW} + c_W^2 C_{HW}\). More...
 
double CHWHB_gagaorth
 The combination of dimension-6 operator coefficients \(-c_W^2 C_{HW} + s_W^2 C_{HW}\). More...
 
double CidH_11r
 
double CidH_22r
 
double CidH_33r
 
double CiDHB
 
double CiDHW
 
double CieH_11r
 
double CieH_22r
 
double CieH_33r
 
double CiH
 
double CiHB
 
double CiHbox
 
double CiHD
 
double CiHd_11
 
double CiHd_22
 
double CiHd_33
 
double CiHe_11
 
double CiHe_22
 
double CiHe_33
 
double CiHL1_11
 
double CiHL1_22
 
double CiHL1_33
 
double CiHL3_11
 
double CiHL3_22
 
double CiHL3_33
 
double CiHQ1_11
 
double CiHQ1_22
 
double CiHQ1_33
 
double CiHQ3_11
 
double CiHQ3_22
 
double CiHQ3_33
 
double CiHu_11
 
double CiHu_22
 
double CiHu_33
 
double CiHW
 
double CiHWB
 
double CiLL_1221
 
double CiLL_2112
 
double CiuB_11r
 
double CiuB_22r
 
double CiuB_33r
 
double CiuG_11r
 
double CiuG_22r
 
double CiuG_33r
 
double CiuH_11r
 
double CiuH_22r
 
double CiuH_33r
 
double CiuW_11r
 
double CiuW_22r
 
double CiuW_33r
 
double CiW
 
double CLd_1111
 
double CLd_1122
 
double CLd_1123
 
double CLd_1132
 
double CLd_1133
 
double CLd_2211
 
double CLd_2223
 
double CLd_2232
 
double CLd_3311
 
double CLd_3323
 
double CLd_3332
 
double CLe_1111
 
double CLe_1122
 
double CLe_1133
 
double CLe_2211
 
double CLe_3311
 
double CLedQ_11
 
double CLedQ_22
 
double cLH3d62
 Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 interactions modifying the Higgs trilinear coupling (Quadratic terms). More...
 
double cLHd6
 Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 interactions. More...
 
double CLL_1111
 
double CLL_1122
 
double CLL_1133
 
double CLL_1221
 
double CLL_1331
 
double CLL_2112
 
double CLL_2211
 
double CLL_3113
 
double CLL_3311
 
double CLQ1_1111
 
double CLQ1_1122
 
double CLQ1_1123
 
double CLQ1_1132
 
double CLQ1_1133
 
double CLQ1_1221
 
double CLQ1_1331
 
double CLQ1_2112
 
double CLQ1_2211
 
double CLQ1_2223
 
double CLQ1_2232
 
double CLQ1_3113
 
double CLQ1_3311
 
double CLQ1_3323
 
double CLQ1_3332
 
double CLQ3_1111
 
double CLQ3_1122
 
double CLQ3_1123
 
double CLQ3_1132
 
double CLQ3_1133
 
double CLQ3_1221
 
double CLQ3_1331
 
double CLQ3_2112
 
double CLQ3_2211
 
double CLQ3_2223
 
double CLQ3_2232
 
double CLQ3_3113
 
double CLQ3_3311
 
double CLQ3_3323
 
double CLQ3_3332
 
double CLu_1111
 
double CLu_1122
 
double CLu_1133
 
double CLu_2211
 
double CLu_2233
 
double CLu_3311
 
double CpLedQ_11
 
double CpLedQ_22
 
double CQe_1111
 
double CQe_1122
 
double CQe_1133
 
double CQe_2211
 
double CQe_2311
 
double CQe_2322
 
double CQe_2333
 
double CQe_3211
 
double CQe_3222
 
double CQe_3233
 
double CQe_3311
 
double CT
 The dimension-6 operator coefficient \(C_{T}\). More...
 
double CuB_11i
 The dimension-6 operator coefficient \((C_{uB})_{11}\) (imaginary part). More...
 
double CuB_11r
 The dimension-6 operator coefficient \((C_{uB})_{11}\) (real part). More...
 
double CuB_12i
 The dimension-6 operator coefficient \((C_{uB})_{12}\) (imaginary part). More...
 
double CuB_12r
 The dimension-6 operator coefficient \((C_{uB})_{12}\) (real part). More...
 
double CuB_13i
 The dimension-6 operator coefficient \((C_{uB})_{13}\) (imaginary part). More...
 
double CuB_13r
 The dimension-6 operator coefficient \((C_{uB})_{13}\) (real part). More...
 
double CuB_22i
 The dimension-6 operator coefficient \((C_{uB})_{22}\) (imaginary part). More...
 
double CuB_22r
 The dimension-6 operator coefficient \((C_{uB})_{22}\) (real part). More...
 
double CuB_23i
 The dimension-6 operator coefficient \((C_{uB})_{23}\) (imaginary part). More...
 
double CuB_23r
 The dimension-6 operator coefficient \((C_{uB})_{23}\) (real part). More...
 
double CuB_33i
 The dimension-6 operator coefficient \((C_{uB})_{33}\) (imaginary part). More...
 
double CuB_33r
 The dimension-6 operator coefficient \((C_{uB})_{33}\) (real part). More...
 
double CuG_11i
 The dimension-6 operator coefficient \((C_{uG})_{11}\) (imaginary part). More...
 
double CuG_11r
 The dimension-6 operator coefficient \((C_{uG})_{11}\) (real part). More...
 
double CuG_12i
 The dimension-6 operator coefficient \((C_{uG})_{12}\) (imaginary part). More...
 
double CuG_12r
 The dimension-6 operator coefficient \((C_{uG})_{12}\) (real part). More...
 
double CuG_13i
 The dimension-6 operator coefficient \((C_{uG})_{13}\) (imaginary part). More...
 
double CuG_13r
 The dimension-6 operator coefficient \((C_{uG})_{13}\) (real part). More...
 
double CuG_22i
 The dimension-6 operator coefficient \((C_{uG})_{22}\) (imaginary part). More...
 
double CuG_22r
 The dimension-6 operator coefficient \((C_{uG})_{22}\) (real part). More...
 
double CuG_23i
 The dimension-6 operator coefficient \((C_{uG})_{23}\) (imaginary part). More...
 
double CuG_23r
 The dimension-6 operator coefficient \((C_{uG})_{23}\) (real part). More...
 
double CuG_33i
 The dimension-6 operator coefficient \((C_{uG})_{33}\) (imaginary part). More...
 
double CuG_33r
 The dimension-6 operator coefficient \((C_{uG})_{33}\) (real part). More...
 
double CuH_11i
 The dimension-6 operator coefficient \((C_{uH})_{11}\) (imaginary part). More...
 
double CuH_11r
 The dimension-6 operator coefficient \((C_{uH})_{11}\) (real part). More...
 
double CuH_12i
 The dimension-6 operator coefficient \((C_{uH})_{12}\) (imaginary part). More...
 
double CuH_12r
 The dimension-6 operator coefficient \((C_{uH})_{12}\) (real part). More...
 
double CuH_13i
 The dimension-6 operator coefficient \((C_{uH})_{13}\) (imaginary part). More...
 
double CuH_13r
 The dimension-6 operator coefficient \((C_{uH})_{13}\) (real part). More...
 
double CuH_22i
 The dimension-6 operator coefficient \((C_{uH})_{22}\) (imaginary part). More...
 
double CuH_22r
 The dimension-6 operator coefficient \((C_{uH})_{22}\) (real part). More...
 
double CuH_23i
 The dimension-6 operator coefficient \((C_{uH})_{23}\) (imaginary part). More...
 
double CuH_23r
 The dimension-6 operator coefficient \((C_{uH})_{23}\) (real part). More...
 
double CuH_33i
 The dimension-6 operator coefficient \((C_{uH})_{33}\) (imaginary part). More...
 
double CuH_33r
 The dimension-6 operator coefficient \((C_{uH})_{33}\) (real part). More...
 
double CuW_11i
 The dimension-6 operator coefficient \((C_{uW})_{11}\) (imaginary part). More...
 
double CuW_11r
 The dimension-6 operator coefficient \((C_{uW})_{11}\) (real part). More...
 
double CuW_12i
 The dimension-6 operator coefficient \((C_{uW})_{12}\) (imaginary part). More...
 
double CuW_12r
 The dimension-6 operator coefficient \((C_{uW})_{12}\) (real part). More...
 
double CuW_13i
 The dimension-6 operator coefficient \((C_{uW})_{13}\) (imaginary part). More...
 
double CuW_13r
 The dimension-6 operator coefficient \((C_{uW})_{13}\) (real part). More...
 
double CuW_22i
 The dimension-6 operator coefficient \((C_{uW})_{22}\) (imaginary part). More...
 
double CuW_22r
 The dimension-6 operator coefficient \((C_{uW})_{22}\) (real part). More...
 
double CuW_23i
 The dimension-6 operator coefficient \((C_{uW})_{23}\) (imaginary part). More...
 
double CuW_23r
 The dimension-6 operator coefficient \((C_{uW})_{23}\) (real part). More...
 
double CuW_33i
 The dimension-6 operator coefficient \((C_{uW})_{33}\) (imaginary part). More...
 
double CuW_33r
 The dimension-6 operator coefficient \((C_{uW})_{33}\) (real part). More...
 
double CW
 The dimension-6 operator coefficient \(C_{W}\). More...
 
double cW2_tree
 The square of the tree level values for the cosine of the weak angle. More...
 
double cW_tree
 The tree level values for the cosine of the weak angle. More...
 
double delta_AA
 Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition. More...
 
double delta_AZ
 Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition. More...
 
double delta_h
 Combinations of dimension 6 coefficients modifying the \(H\) canonical field definition. More...
 
double delta_ZZ
 Combination of dimension 6 coefficients modifying the \(Z_\mu\) canonical field definition. More...
 
double dg1Z
 Independent contribution to aTGC. More...
 
double dGammaHTotR1
 
double dGammaHTotR2
 
double dKappaga
 Independent contribution to aTGC.
More...
 
double dZH
 Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization. More...
 
double eeettHint
 Intrinsic relative theoretical error in \(e^+ e^- \to t \bar{t} H\). (Assumed to be constant in energy.) More...
 
double eeettHpar
 Parametric relative theoretical error in \(e^+ e^- \to t \bar{t} H\). (Assumed to be constant in energy.) More...
 
double eeeWBFint
 Intrinsic relative theoretical error in \(e^+ e^- \to H \bar{\nu} \nu\). (Assumed to be constant in energy.) More...
 
double eeeWBFpar
 Parametric relative theoretical error in \(e^+ e^- \to H \bar{\nu} \nu\). (Assumed to be constant in energy.) More...
 
double eeeZHint
 Intrinsic relative theoretical error in \(e^+ e^- \to Z H\). (Assumed to be constant in energy.) More...
 
double eeeZHpar
 Parametric relative theoretical error in \(e^+ e^- \to Z H\). (Assumed to be constant in energy.) More...
 
double eeMz
 The em coupling at Mz. More...
 
double eeMz2
 The em coupling squared (at Mz). More...
 
double eepWBFint
 Intrinsic relative theoretical error in \(e^- p \to H e^- j\) via WBF. (Assumed to be constant in energy.) More...
 
double eepWBFpar
 Parametric relative theoretical error in \(e^- p \to H e^- j\) via WBF. (Assumed to be constant in energy.)
More...
 
double eepZBFint
 Intrinsic relative theoretical error in \(e^- p \to H e^- j\) via ZBF. (Assumed to be constant in energy.) More...
 
double eepZBFpar
 Parametric relative theoretical error in \(e^- p \to H e^- j\) via ZBF. (Assumed to be constant in energy.) More...
 
double eggFHbb
 
double eggFHgaga
 
double eggFHmumu
 Total relative theoretical error in \(gg \to H \to X\).
More...
 
double eggFHtautau
 
double eggFHWW
 
double eggFHZga
 
double eggFHZZ
 
double eggFint
 Intrinsic relative theoretical error in ggF production. (Assumed to be constant in energy.) More...
 
double eggFpar
 Parametric relative theoretical error in ggF production. (Assumed to be constant in energy.) More...
 
double eHbbint
 Intrinsic relative theoretical error in \(H \to b\bar{b}\). More...
 
double eHbbpar
 Parametric relative theoretical error in \(H \to b\bar{b}\). More...
 
double eHccint
 Intrinsic relative theoretical error in \(H \to c\bar{c}\). More...
 
double eHccpar
 Parametric relative theoretical error in \(H \to c\bar{c}\). More...
 
double eHgagaint
 Intrinsic relative theoretical error in \(H \to \gamma\gamma\). More...
 
double eHgagapar
 Parametric relative theoretical error in \(H \to \gamma\gamma\). More...
 
double eHggint
 Intrinsic relative theoretical error in \(H \to g g\). More...
 
double eHggpar
 Parametric relative theoretical error in \(H \to g g\). More...
 
double eHmumuint
 Intrinsic relative theoretical error in \(H \to \mu^+ \mu^-\). More...
 
double eHmumupar
 Parametric relative theoretical error in \(H \to \mu^+ \mu^-\). More...
 
double eHtautauint
 Intrinsic relative theoretical error in \(H \to \tau^+ \tau^-\). More...
 
double eHtautaupar
 Parametric relative theoretical error in \(H \to \tau^+ \tau^-\). More...
 
double eHwidth
 Total relative theoretical error in the Higgs width. More...
 
double eHWWint
 Intrinsic relative theoretical error in \(H \to W W\). More...
 
double eHWWpar
 Parametric relative theoretical error in \(H \to W W\). More...
 
double eHZgaint
 Intrinsic relative theoretical error in \(H \to Z \gamma\). More...
 
double eHZgapar
 Parametric relative theoretical error in \(H \to Z \gamma\). More...
 
double eHZZint
 Intrinsic relative theoretical error in \(H \to Z Z\). More...
 
double eHZZpar
 Parametric relative theoretical error in \(H \to Z Z\). More...
 
double ettH_1314_DeltagHt
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (13 & 14 TeV). More...
 
double ettH_1314_G
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (13 & 14 TeV). More...
 
double ettH_1314_HG
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (13 & 14 TeV). More...
 
double ettH_1314_uG_33r
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (13 & 14 TeV). More...
 
double ettH_2_DeltagHt
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (1.96 TeV). More...
 
double ettH_2_G
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (1.96 TeV). More...
 
double ettH_2_HG
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (1.96 TeV). More...
 
double ettH_2_uG_33r
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (1.96 TeV). More...
 
double ettH_78_DeltagHt
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (7 & 8 TeV). More...
 
double ettH_78_G
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (7 & 8 TeV). More...
 
double ettH_78_HG
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (7 & 8 TeV). More...
 
double ettH_78_uG_33r
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (7 & 8 TeV). More...
 
double ettHbb
 
double ettHgaga
 
double ettHint
 Intrinsic relative theoretical error in ttH production. (Assumed to be constant in energy.) More...
 
double ettHmumu
 Total relative theoretical error in \(pp \to ttH \to tt X\). More...
 
double ettHpar
 Parametric relative theoretical error in ttH production. (Assumed to be constant in energy.) More...
 
double ettHtautau
 
double ettHWW
 
double ettHZga
 
double ettHZZ
 
double eVBF_1314_DeltaGF
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_DHB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_DHW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_HB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_Hbox
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_HD
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_Hd_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_HG
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_HQ1_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_HQ3_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_Hu_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_HW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_HWB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_2_DeltaGF
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_DHB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_DHW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_HB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_Hbox
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_HD
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_Hd_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_HG
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_HQ1_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_HQ3_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_Hu_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_HW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_HWB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_78_DeltaGF
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_DHB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_DHW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_HB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_Hbox
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_HD
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_Hd_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_HG
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_HQ1_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_HQ3_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_Hu_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_HW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_HWB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBFHbb
 
double eVBFHgaga
 
double eVBFHinv
 
double eVBFHmumu
 Total relative theoretical error in \(pp \to Hjj (VBF) \to X jj\).
More...
 
double eVBFHtautau
 
double eVBFHWW
 
double eVBFHZga
 
double eVBFHZZ
 
double eVBFint
 Intrinsic relative theoretical error in VBF production. (Assumed to be constant in energy.) More...
 
double eVBFpar
 Parametric relative theoretical error in VBF production. (Assumed to be constant in energy.) More...
 
double eVHinv
 Total relative theoretical error in \(pp \to X H \to X + invisible\). More...
 
double eWH_1314_DeltaGF
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (13 & 14 TeV). More...
 
double eWH_1314_DHW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (13 & 14 TeV). More...
 
double eWH_1314_Hbox
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (13 & 14 TeV). More...
 
double eWH_1314_HD
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (13 & 14 TeV). More...
 
double eWH_1314_HQ3_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (13 & 14 TeV). More...
 
double eWH_1314_HW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (13 & 14 TeV). More...
 
double eWH_1314_HWB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (13 & 14 TeV). More...
 
double eWH_2_DeltaGF
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (1.96 TeV). More...
 
double eWH_2_DHW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (1.96 TeV). More...
 
double eWH_2_Hbox
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (1.96 TeV). More...
 
double eWH_2_HD
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (1.96 TeV). More...
 
double eWH_2_HQ3_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (1.96 TeV). More...
 
double eWH_2_HW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (1.96 TeV). More...
 
double eWH_2_HWB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (1.96 TeV). More...
 
double eWH_78_DeltaGF
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (7 & 8 TeV). More...
 
double eWH_78_DHW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (7 & 8 TeV). More...
 
double eWH_78_Hbox
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (7 & 8 TeV). More...
 
double eWH_78_HD
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (7 & 8 TeV). More...
 
double eWH_78_HQ3_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (7 & 8 TeV). More...
 
double eWH_78_HW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (7 & 8 TeV). More...
 
double eWH_78_HWB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (7 & 8 TeV). More...
 
double eWHbb
 
double eWHgaga
 
double eWHint
 Intrinsic relative theoretical error in WH production. (Assumed to be constant in energy.) More...
 
double eWHmumu
 Total relative theoretical error in \(pp \to WH \to W X\).
More...
 
double eWHpar
 Parametric relative theoretical error in WH production. (Assumed to be constant in energy.) More...
 
double eWHtautau
 
double eWHWW
 
double eWHZga
 
double eWHZZ
 
double eZH_1314_DeltaGF
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_DHB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_DHW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_HB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_Hbox
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_HD
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_Hd_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_HQ1_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_HQ3_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_Hu_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_HW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_HWB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_2_DeltaGF
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_DHB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_DHW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_HB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_Hbox
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_HD
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_Hd_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_HQ1_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_HQ3_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_Hu_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_HW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_HWB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_78_DeltaGF
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_DHB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_DHW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_HB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_Hbox
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_HD
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_Hd_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_HQ1_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_HQ3_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_Hu_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_HW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_HWB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZHbb
 
double eZHgaga
 
double eZHint
 Intrinsic relative theoretical error in ZH production. (Assumed to be constant in energy.) More...
 
double eZHmumu
 Total relative theoretical error in \(pp \to ZH \to Z X\). More...
 
double eZHpar
 Parametric relative theoretical error in ZH production. (Assumed to be constant in energy.) More...
 
double eZHtautau
 
double eZHWW
 
double eZHZga
 
double eZHZZ
 
double g1_tree
 The tree level value of the \(U(1)_Y\) gauge coupling contant (at the \(Z\) pole). More...
 
double g2_tree
 The tree level value of the \(SU(2)_L\) gauge coupling contant (at the \(Z\) pole). More...
 
double g3_tree
 The tree level value of the \(SU(3)_c\) gauge coupling contant (at the \(Z\) pole). More...
 
double GammaHTotR
 NP contributions and Total to Higgs width ratio with SM. More...
 
double gZdL
 
double gZdR
 The tree level value of the \(Z\bar{d}d\) couplings in the SM. More...
 
double gZlL
 
double gZlR
 The tree level value of the \(Z\ell^+\ell^-\) couplings in the SM. More...
 
double gZuL
 
double gZuR
 The tree level value of the \(Z\bar{u}u\) couplings in the SM. More...
 
double gZvL
 The tree level value of the \(Z\bar{\nu}\nu\) couplings in the SM. More...
 
double Lambda_NP
 The new physics scale [GeV]. More...
 
double lambdaH_tree
 The SM tree level value of the scalar quartic coupling in the potential. More...
 
double LambdaNP2
 The square of the new physics scale [GeV \(^2\)]. More...
 
double lambZ
 Independent contribution to aTGC. More...
 
Matching< NPSMEFTd6Matching, NPSMEFTd6NPSMEFTd6M
 
double sW2_tree
 The square of the tree level values for the sine of the weak angle. More...
 
double sW_tree
 The tree level values for the sine of the weak angle. More...
 
double UevL
 The tree level value of the \(W^-\bar{\ell}\nu\) couplings in the SM. (Neglecting PMNS effects.) More...
 
double v2
 The square of the EW vev. More...
 
double v2_over_LambdaNP2
 The ratio between the EW vev and the new physics scale, squared \(v^2/\Lambda^2\). More...
 
double VudL
 The tree level value of the \(W^+\bar{u}d\) couplings in the SM. (Neglecting CKM effects.) More...
 
double Yukb
 SM d-quark Yukawas. More...
 
double Yukc
 
double Yukd
 
double Yuke
 
double Yukmu
 
double Yuks
 
double Yukt
 SM u-quark Yukawas. More...
 
double Yuktau
 SM lepton Yukawas. More...
 
double Yuku
 
- Protected Attributes inherited from NPbase
StandardModel trueSM
 
- Protected Attributes inherited from StandardModel
double A
 The CKM parameter \(A\) in the Wolfenstein parameterization. More...
 
double ale
 The fine-structure constant \(\alpha\). More...
 
double alpha21
 
double alpha31
 
double AlsMz
 The strong coupling constant at the Z-boson mass, \(\alpha_s(M_Z)\). More...
 
double dAle5Mz
 The five-flavour hadronic contribution to the electromagnetic coupling, \(\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)\). More...
 
double delGammaZ
 The theoretical uncertainty in \(\Gamma_Z\), denoted as \(\delta\,\Gamma_Z\), in GeV. More...
 
double delMw
 The theoretical uncertainty in \(M_W\), denoted as \(\delta\,M_W\), in GeV. More...
 
double delR0b
 The theoretical uncertainty in \(R_b^0\), denoted as \(\delta\,R_b^0\). More...
 
double delR0c
 The theoretical uncertainty in \(R_c^0\), denoted as \(\delta\,R_c^0\). More...
 
double delR0l
 The theoretical uncertainty in \(R_l^0\), denoted as \(\delta\,R_l^0\). More...
 
double delsigma0H
 The theoretical uncertainty in \(\sigma_{Hadron}^0\), denoted as \(\delta\,\sigma_{Hadron}^0\) in nb. More...
 
double delSin2th_b
 The theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{b}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{b}\). More...
 
double delSin2th_l
 The theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{\rm lept}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{\rm lept}\). More...
 
double delSin2th_q
 The theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{q\not = b,t}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{q\not = b,t}\). More...
 
double delta
 
double etab
 The CKM parameter \(\bar{\eta}\) in the Wolfenstein parameterization. More...
 
bool flag_order [orders_EW_size]
 An array of internal flags controlling the inclusions of higher-order corrections. More...
 
double gamma
 \(\gamma \) used as an input for FlagWolfenstein = FALSE More...
 
double GF
 The Fermi constant \(G_\mu\) in \({\rm GeV}^{-2}\). More...
 
double lambda
 The CKM parameter \(\lambda\) in the Wolfenstein parameterization. More...
 
Particle leptons [6]
 An array of Particle objects for the leptons. More...
 
double mHl
 The Higgs mass \(m_h\) in GeV. More...
 
double muw
 A matching scale \(\mu_W\) around the weak scale in GeV. More...
 
CKM myCKM
 An object of type CKM. More...
 
PMNS myPMNS
 
double Mz
 The mass of the \(Z\) boson in GeV. More...
 
bool requireCKM
 An internal flag to control whether the CKM matrix has to be recomputed. More...
 
bool requireYe
 An internal flag to control whether the charged-lepton Yukawa matrix has to be recomputed. More...
 
bool requireYn
 An internal flag to control whether the neutrino Yukawa matrix has to be recomputed. More...
 
double rhob
 The CKM parameter \(\bar{\rho}\) in the Wolfenstein parameterization. More...
 
double s12
 
double s13
 
double s23
 
Flavour SMFlavour
 An object of type Flavour. More...
 
Matching< StandardModelMatching, StandardModelSMM
 An object of type Matching. More...
 
double Vcb
 \(\vert V_{cb} \vert \) used as an input for FlagWolfenstein = FALSE More...
 
double Vub
 \(\vert V_{ub} \vert \) used as an input for FlagWolfenstein = FALSE More...
 
double Vus
 \(\vert V_{us} \vert \) used as an input for FlagWolfenstein = FALSE More...
 
gslpp::matrix< gslpp::complexYd
 The Yukawa matrix of the down-type quarks. More...
 
gslpp::matrix< gslpp::complexYe
 The Yukawa matrix of the charged leptons. More...
 
gslpp::matrix< gslpp::complexYn
 The Yukawa matrix of the neutrinos. More...
 
gslpp::matrix< gslpp::complexYu
 The Yukawa matrix of the up-type quarks. More...
 
- Protected Attributes inherited from QCD
double AlsM
 The strong coupling constant at the mass scale MAls, \(\alpha_s(M_{\alpha_s})\). More...
 
double CA
 
double CF
 
bool computemt
 Switch for computing the \(\overline{\mathrm{MS}}\) mass of the top quark. More...
 
double dAdA_NA
 
double dFdA_NA
 
double dFdF_NA
 
double MAls
 The mass scale in GeV at which the strong coupling measurement is provided. More...
 
double mtpole
 The pole mass of the top quark. More...
 
double mub
 The threshold between five- and four-flavour theory in GeV. More...
 
double muc
 The threshold between four- and three-flavour theory in GeV. More...
 
double mut
 The threshold between six- and five-flavour theory in GeV. More...
 
double NA
 
double Nc
 The number of colours. More...
 
Particle quarks [6]
 The vector of all SM quarks. More...
 
bool requireYd
 Switch for generating the Yukawa couplings to the down-type quarks. More...
 
bool requireYu
 Switch for generating the Yukawa couplings to the up-type quarks. More...
 
double TF
 
- Protected Attributes inherited from Model
bool isSliced
 A boolean set to true if the current istance is a slice of an extended object. More...
 
std::map< std::string, std::reference_wrapper< const double > > ModelParamMap
 
bool UpdateError
 A boolean set to false if update is successful. More...
 

Private Attributes

bool FlagFlavU3OfX
 A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients. More...
 
bool FlagHiggsSM
 A boolean flag that is true if including dependence on small variations of the SM parameters (dependence is linearized). Available only in selected Higgs observables. More...
 
const bool FlagLeptonUniversal
 An internal boolean flag that is true if assuming lepton flavour universality. More...
 
bool FlagLoopH3d6Quad
 A boolean flag that is true if including quadratic modifications in the SM loops in Higgs observables due to the dim 6 interactions that contribute to the trilinear Higgs coupling. More...
 
bool FlagLoopHd6
 A boolean flag that is true if including modifications in the SM loops in Higgs observables due to the dim 6 interactions. More...
 
bool FlagPartialQFU
 A boolean flag that is true if assuming partial quark flavour universality between the 1st and 2nd family in the CHF operators. More...
 
bool FlagQuadraticTerms
 A boolean flag that is true if the quadratic terms in cross sections and widths are switched on. More...
 
const bool FlagQuarkUniversal
 An internal boolean flag that is true if assuming quark flavour universality. More...
 
bool FlagRotateCHWCHB
 A boolean flag that is true if we use as parameters CHWHB_gaga and CHWHB_gagaorth instead of CHW and CHB. More...
 
bool FlagUnivOfX
 A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients and all proportional to the same coefficient (CuH_33 and CuV_33 respectively). More...
 
gsl_integration_cquad_workspace * w_WW
 

Additional Inherited Members

- Public Types inherited from StandardModel
enum  LEP2RCs { Weak = 0, WeakBox, ISR, QEDFSR, QCDFSR, NUMofLEP2RCs }
 
enum  orders_EW { EW1 = 0, EW1QCD1, EW1QCD2, EW2, EW2QCD1, EW3, orders_EW_size }
 An enumerated type representing perturbative orders of radiative corrections to EW precision observables. More...
 
- Public Types inherited from QCD
enum  lepton { NEUTRINO_1, ELECTRON, NEUTRINO_2, MU, NEUTRINO_3, TAU, NOLEPTON }
 An enum type for leptons. More...
 
enum  meson { P_0, P_P, K_0, K_P, D_0, D_P, B_D, B_P, B_S, B_C, PHI, K_star, K_star_P, D_star_P, RHO, RHO_P, OMEGA, MESON_END }
 An enum type for mesons. More...
 
enum  quark { UP, DOWN, CHARM, STRANGE, TOP, BOTTOM }
 An enum type for quarks. More...
 

Constructor & Destructor Documentation

◆ NPSMEFTd6()

NPSMEFTd6::NPSMEFTd6 ( const bool  FlagLeptonUniversal_in = false,
const bool  FlagQuarkUniversal_in = false 
)

Constructor.

Parameters
[in]FlagLeptonUniversal_inan internal boolean flag that is true if assuming lepton flavour universality
[in]FlagQuarkUniversal_inan internal boolean flag that is true if assuming quark flavour universality

Definition at line 280 of file NPSMEFTd6.cpp.

281 : NPbase(), NPSMEFTd6M(*this), FlagLeptonUniversal(FlagLeptonUniversal_in), FlagQuarkUniversal(FlagQuarkUniversal_in)
282 {
285  throw std::runtime_error("Invalid arguments for NPSMEFTd6::NPSMEFTd6()");
286 
287  FlagQuadraticTerms = false;
288  FlagRotateCHWCHB = false;
289  FlagPartialQFU = false;
290  FlagFlavU3OfX = false;
291  FlagUnivOfX = false;
292  FlagHiggsSM = false;
293  FlagLoopHd6 = false;
294  FlagLoopH3d6Quad = false;
296 
297  w_WW = gsl_integration_cquad_workspace_alloc(100);
298 
300 
301  ModelParamMap.insert(std::make_pair("CG", std::cref(CG)));
302  ModelParamMap.insert(std::make_pair("CW", std::cref(CW)));
303  ModelParamMap.insert(std::make_pair("C2B", std::cref(C2B)));
304  ModelParamMap.insert(std::make_pair("C2W", std::cref(C2W)));
305  ModelParamMap.insert(std::make_pair("C2BS", std::cref(C2BS)));
306  ModelParamMap.insert(std::make_pair("C2WS", std::cref(C2WS)));
307  ModelParamMap.insert(std::make_pair("CHG", std::cref(CHG)));
308  ModelParamMap.insert(std::make_pair("CHW", std::cref(CHW)));
309  ModelParamMap.insert(std::make_pair("CHB", std::cref(CHB)));
310  ModelParamMap.insert(std::make_pair("CHWHB_gaga", std::cref(CHWHB_gaga)));
311  ModelParamMap.insert(std::make_pair("CHWHB_gagaorth", std::cref(CHWHB_gagaorth)));
312  ModelParamMap.insert(std::make_pair("CDHB", std::cref(CDHB)));
313  ModelParamMap.insert(std::make_pair("CDHW", std::cref(CDHW)));
314  ModelParamMap.insert(std::make_pair("CDB", std::cref(CDB)));
315  ModelParamMap.insert(std::make_pair("CDW", std::cref(CDW)));
316  ModelParamMap.insert(std::make_pair("CHWB", std::cref(CHWB)));
317  ModelParamMap.insert(std::make_pair("CHD", std::cref(CHD)));
318  ModelParamMap.insert(std::make_pair("CT", std::cref(CT)));
319  ModelParamMap.insert(std::make_pair("CHbox", std::cref(CHbox)));
320  ModelParamMap.insert(std::make_pair("CH", std::cref(CH)));
321  if (FlagLeptonUniversal) {
322  ModelParamMap.insert(std::make_pair("CHL1", std::cref(CHL1_11)));
323  ModelParamMap.insert(std::make_pair("CHL3", std::cref(CHL3_11)));
324  ModelParamMap.insert(std::make_pair("CHe", std::cref(CHe_11)));
325  ModelParamMap.insert(std::make_pair("CeH_11r", std::cref(CeH_11r)));
326  ModelParamMap.insert(std::make_pair("CeH_22r", std::cref(CeH_22r)));
327  ModelParamMap.insert(std::make_pair("CeH_33r", std::cref(CeH_33r)));
328  ModelParamMap.insert(std::make_pair("CeH_11i", std::cref(CeH_11i)));
329  ModelParamMap.insert(std::make_pair("CeH_22i", std::cref(CeH_22i)));
330  ModelParamMap.insert(std::make_pair("CeH_33i", std::cref(CeH_33i)));
331  ModelParamMap.insert(std::make_pair("CLL", std::cref(CLL_1221)));
332  ModelParamMap.insert(std::make_pair("Cee", std::cref(Cee_1111)));
333  ModelParamMap.insert(std::make_pair("CLe", std::cref(CLe_1111)));
334  } else {
335  ModelParamMap.insert(std::make_pair("CHL1_11", std::cref(CHL1_11)));
336  ModelParamMap.insert(std::make_pair("CHL1_12r", std::cref(CHL1_12r)));
337  ModelParamMap.insert(std::make_pair("CHL1_13r", std::cref(CHL1_13r)));
338  ModelParamMap.insert(std::make_pair("CHL1_22", std::cref(CHL1_22)));
339  ModelParamMap.insert(std::make_pair("CHL1_23r", std::cref(CHL1_23r)));
340  ModelParamMap.insert(std::make_pair("CHL1_33", std::cref(CHL1_33)));
341  ModelParamMap.insert(std::make_pair("CHL1_12i", std::cref(CHL1_12i)));
342  ModelParamMap.insert(std::make_pair("CHL1_13i", std::cref(CHL1_13i)));
343  ModelParamMap.insert(std::make_pair("CHL1_23i", std::cref(CHL1_23i)));
344  ModelParamMap.insert(std::make_pair("CHL3_11", std::cref(CHL3_11)));
345  ModelParamMap.insert(std::make_pair("CHL3_12r", std::cref(CHL3_12r)));
346  ModelParamMap.insert(std::make_pair("CHL3_13r", std::cref(CHL3_13r)));
347  ModelParamMap.insert(std::make_pair("CHL3_22", std::cref(CHL3_22)));
348  ModelParamMap.insert(std::make_pair("CHL3_23r", std::cref(CHL3_23r)));
349  ModelParamMap.insert(std::make_pair("CHL3_33", std::cref(CHL3_33)));
350  ModelParamMap.insert(std::make_pair("CHL3_12i", std::cref(CHL3_12i)));
351  ModelParamMap.insert(std::make_pair("CHL3_13i", std::cref(CHL3_13i)));
352  ModelParamMap.insert(std::make_pair("CHL3_23i", std::cref(CHL3_23i)));
353  ModelParamMap.insert(std::make_pair("CHe_11", std::cref(CHe_11)));
354  ModelParamMap.insert(std::make_pair("CHe_12r", std::cref(CHe_12r)));
355  ModelParamMap.insert(std::make_pair("CHe_13r", std::cref(CHe_13r)));
356  ModelParamMap.insert(std::make_pair("CHe_22", std::cref(CHe_22)));
357  ModelParamMap.insert(std::make_pair("CHe_23r", std::cref(CHe_23r)));
358  ModelParamMap.insert(std::make_pair("CHe_33", std::cref(CHe_33)));
359  ModelParamMap.insert(std::make_pair("CHe_12i", std::cref(CHe_12i)));
360  ModelParamMap.insert(std::make_pair("CHe_13i", std::cref(CHe_13i)));
361  ModelParamMap.insert(std::make_pair("CHe_23i", std::cref(CHe_23i)));
362  ModelParamMap.insert(std::make_pair("CeH_11r", std::cref(CeH_11r)));
363  ModelParamMap.insert(std::make_pair("CeH_12r", std::cref(CeH_12r)));
364  ModelParamMap.insert(std::make_pair("CeH_13r", std::cref(CeH_13r)));
365  ModelParamMap.insert(std::make_pair("CeH_22r", std::cref(CeH_22r)));
366  ModelParamMap.insert(std::make_pair("CeH_23r", std::cref(CeH_23r)));
367  ModelParamMap.insert(std::make_pair("CeH_33r", std::cref(CeH_33r)));
368  ModelParamMap.insert(std::make_pair("CeH_11i", std::cref(CeH_11i)));
369  ModelParamMap.insert(std::make_pair("CeH_12i", std::cref(CeH_12i)));
370  ModelParamMap.insert(std::make_pair("CeH_13i", std::cref(CeH_13i)));
371  ModelParamMap.insert(std::make_pair("CeH_22i", std::cref(CeH_22i)));
372  ModelParamMap.insert(std::make_pair("CeH_23i", std::cref(CeH_23i)));
373  ModelParamMap.insert(std::make_pair("CeH_33i", std::cref(CeH_33i)));
374  ModelParamMap.insert(std::make_pair("CLL_1111", std::cref(CLL_1111)));
375  ModelParamMap.insert(std::make_pair("CLL_1221", std::cref(CLL_1221)));
376  ModelParamMap.insert(std::make_pair("CLL_1122", std::cref(CLL_1122)));
377  ModelParamMap.insert(std::make_pair("CLL_1331", std::cref(CLL_1331)));
378  ModelParamMap.insert(std::make_pair("CLL_1133", std::cref(CLL_1133)));
379  ModelParamMap.insert(std::make_pair("Cee_1111", std::cref(Cee_1111)));
380  ModelParamMap.insert(std::make_pair("Cee_1122", std::cref(Cee_1122)));
381  ModelParamMap.insert(std::make_pair("Cee_1133", std::cref(Cee_1133)));
382  ModelParamMap.insert(std::make_pair("CLe_1111", std::cref(CLe_1111)));
383  ModelParamMap.insert(std::make_pair("CLe_1122", std::cref(CLe_1122)));
384  ModelParamMap.insert(std::make_pair("CLe_2211", std::cref(CLe_2211)));
385  ModelParamMap.insert(std::make_pair("CLe_1133", std::cref(CLe_1133)));
386  ModelParamMap.insert(std::make_pair("CLe_3311", std::cref(CLe_3311)));
387  }
388  if (FlagQuarkUniversal) {
389  ModelParamMap.insert(std::make_pair("CHQ1", std::cref(CHQ1_11)));
390  ModelParamMap.insert(std::make_pair("CHQ3", std::cref(CHQ3_11)));
391  ModelParamMap.insert(std::make_pair("CHu", std::cref(CHu_11)));
392  ModelParamMap.insert(std::make_pair("CHd", std::cref(CHd_11)));
393  ModelParamMap.insert(std::make_pair("CHud_r", std::cref(CHud_11r)));
394  ModelParamMap.insert(std::make_pair("CHud_i", std::cref(CHud_11i)));
395  ModelParamMap.insert(std::make_pair("CuH_11r", std::cref(CuH_11r)));
396  ModelParamMap.insert(std::make_pair("CuH_22r", std::cref(CuH_22r)));
397  ModelParamMap.insert(std::make_pair("CuH_33r", std::cref(CuH_33r)));
398  ModelParamMap.insert(std::make_pair("CuH_11i", std::cref(CuH_11i)));
399  ModelParamMap.insert(std::make_pair("CuH_22i", std::cref(CuH_22i)));
400  ModelParamMap.insert(std::make_pair("CuH_33i", std::cref(CuH_33i)));
401  ModelParamMap.insert(std::make_pair("CdH_11r", std::cref(CdH_11r)));
402  ModelParamMap.insert(std::make_pair("CdH_22r", std::cref(CdH_22r)));
403  ModelParamMap.insert(std::make_pair("CdH_33r", std::cref(CdH_33r)));
404  ModelParamMap.insert(std::make_pair("CdH_11i", std::cref(CdH_11i)));
405  ModelParamMap.insert(std::make_pair("CdH_22i", std::cref(CdH_22i)));
406  ModelParamMap.insert(std::make_pair("CdH_33i", std::cref(CdH_33i)));
407  ModelParamMap.insert(std::make_pair("CuG_r", std::cref(CuG_11r)));
408  ModelParamMap.insert(std::make_pair("CuG_i", std::cref(CuG_11i)));
409  ModelParamMap.insert(std::make_pair("CuW_r", std::cref(CuW_11r)));
410  ModelParamMap.insert(std::make_pair("CuW_i", std::cref(CuW_11i)));
411  ModelParamMap.insert(std::make_pair("CuB_r", std::cref(CuB_11r)));
412  ModelParamMap.insert(std::make_pair("CuB_i", std::cref(CuB_11i)));
413  } else {
414  ModelParamMap.insert(std::make_pair("CHQ1_11", std::cref(CHQ1_11)));
415  ModelParamMap.insert(std::make_pair("CHQ1_12r", std::cref(CHQ1_12r)));
416  ModelParamMap.insert(std::make_pair("CHQ1_13r", std::cref(CHQ1_13r)));
417  ModelParamMap.insert(std::make_pair("CHQ1_22", std::cref(CHQ1_22)));
418  ModelParamMap.insert(std::make_pair("CHQ1_23r", std::cref(CHQ1_23r)));
419  ModelParamMap.insert(std::make_pair("CHQ1_33", std::cref(CHQ1_33)));
420  ModelParamMap.insert(std::make_pair("CHQ1_12i", std::cref(CHQ1_12i)));
421  ModelParamMap.insert(std::make_pair("CHQ1_13i", std::cref(CHQ1_13i)));
422  ModelParamMap.insert(std::make_pair("CHQ1_23i", std::cref(CHQ1_23i)));
423  ModelParamMap.insert(std::make_pair("CHQ3_11", std::cref(CHQ3_11)));
424  ModelParamMap.insert(std::make_pair("CHQ3_12r", std::cref(CHQ3_12r)));
425  ModelParamMap.insert(std::make_pair("CHQ3_13r", std::cref(CHQ3_13r)));
426  ModelParamMap.insert(std::make_pair("CHQ3_22", std::cref(CHQ3_22)));
427  ModelParamMap.insert(std::make_pair("CHQ3_23r", std::cref(CHQ3_23r)));
428  ModelParamMap.insert(std::make_pair("CHQ3_33", std::cref(CHQ3_33)));
429  ModelParamMap.insert(std::make_pair("CHQ3_12i", std::cref(CHQ3_12i)));
430  ModelParamMap.insert(std::make_pair("CHQ3_13i", std::cref(CHQ3_13i)));
431  ModelParamMap.insert(std::make_pair("CHQ3_23i", std::cref(CHQ3_23i)));
432  ModelParamMap.insert(std::make_pair("CHu_11", std::cref(CHu_11)));
433  ModelParamMap.insert(std::make_pair("CHu_12r", std::cref(CHu_12r)));
434  ModelParamMap.insert(std::make_pair("CHu_13r", std::cref(CHu_13r)));
435  ModelParamMap.insert(std::make_pair("CHu_22", std::cref(CHu_22)));
436  ModelParamMap.insert(std::make_pair("CHu_23r", std::cref(CHu_23r)));
437  ModelParamMap.insert(std::make_pair("CHu_33", std::cref(CHu_33)));
438  ModelParamMap.insert(std::make_pair("CHu_12i", std::cref(CHu_12i)));
439  ModelParamMap.insert(std::make_pair("CHu_13i", std::cref(CHu_13i)));
440  ModelParamMap.insert(std::make_pair("CHu_23i", std::cref(CHu_23i)));
441  ModelParamMap.insert(std::make_pair("CHd_11", std::cref(CHd_11)));
442  ModelParamMap.insert(std::make_pair("CHd_12r", std::cref(CHd_12r)));
443  ModelParamMap.insert(std::make_pair("CHd_13r", std::cref(CHd_13r)));
444  ModelParamMap.insert(std::make_pair("CHd_22", std::cref(CHd_22)));
445  ModelParamMap.insert(std::make_pair("CHd_23r", std::cref(CHd_23r)));
446  ModelParamMap.insert(std::make_pair("CHd_33", std::cref(CHd_33)));
447  ModelParamMap.insert(std::make_pair("CHd_12i", std::cref(CHd_12i)));
448  ModelParamMap.insert(std::make_pair("CHd_13i", std::cref(CHd_13i)));
449  ModelParamMap.insert(std::make_pair("CHd_23i", std::cref(CHd_23i)));
450  ModelParamMap.insert(std::make_pair("CHud_11r", std::cref(CHud_11r)));
451  ModelParamMap.insert(std::make_pair("CHud_12r", std::cref(CHud_12r)));
452  ModelParamMap.insert(std::make_pair("CHud_13r", std::cref(CHud_13r)));
453  ModelParamMap.insert(std::make_pair("CHud_22r", std::cref(CHud_22r)));
454  ModelParamMap.insert(std::make_pair("CHud_23r", std::cref(CHud_23r)));
455  ModelParamMap.insert(std::make_pair("CHud_33r", std::cref(CHud_33r)));
456  ModelParamMap.insert(std::make_pair("CHud_11i", std::cref(CHud_11i)));
457  ModelParamMap.insert(std::make_pair("CHud_12i", std::cref(CHud_12i)));
458  ModelParamMap.insert(std::make_pair("CHud_13i", std::cref(CHud_13i)));
459  ModelParamMap.insert(std::make_pair("CHud_22i", std::cref(CHud_22i)));
460  ModelParamMap.insert(std::make_pair("CHud_23i", std::cref(CHud_23i)));
461  ModelParamMap.insert(std::make_pair("CHud_33i", std::cref(CHud_33i)));
462  ModelParamMap.insert(std::make_pair("CuH_11r", std::cref(CuH_11r)));
463  ModelParamMap.insert(std::make_pair("CuH_12r", std::cref(CuH_12r)));
464  ModelParamMap.insert(std::make_pair("CuH_13r", std::cref(CuH_13r)));
465  ModelParamMap.insert(std::make_pair("CuH_22r", std::cref(CuH_22r)));
466  ModelParamMap.insert(std::make_pair("CuH_23r", std::cref(CuH_23r)));
467  ModelParamMap.insert(std::make_pair("CuH_33r", std::cref(CuH_33r)));
468  ModelParamMap.insert(std::make_pair("CuH_11i", std::cref(CuH_11i)));
469  ModelParamMap.insert(std::make_pair("CuH_12i", std::cref(CuH_12i)));
470  ModelParamMap.insert(std::make_pair("CuH_13i", std::cref(CuH_13i)));
471  ModelParamMap.insert(std::make_pair("CuH_22i", std::cref(CuH_22i)));
472  ModelParamMap.insert(std::make_pair("CuH_23i", std::cref(CuH_23i)));
473  ModelParamMap.insert(std::make_pair("CuH_33i", std::cref(CuH_33i)));
474  ModelParamMap.insert(std::make_pair("CdH_11r", std::cref(CdH_11r)));
475  ModelParamMap.insert(std::make_pair("CdH_12r", std::cref(CdH_12r)));
476  ModelParamMap.insert(std::make_pair("CdH_13r", std::cref(CdH_13r)));
477  ModelParamMap.insert(std::make_pair("CdH_22r", std::cref(CdH_22r)));
478  ModelParamMap.insert(std::make_pair("CdH_23r", std::cref(CdH_23r)));
479  ModelParamMap.insert(std::make_pair("CdH_33r", std::cref(CdH_33r)));
480  ModelParamMap.insert(std::make_pair("CdH_11i", std::cref(CdH_11i)));
481  ModelParamMap.insert(std::make_pair("CdH_12i", std::cref(CdH_12i)));
482  ModelParamMap.insert(std::make_pair("CdH_13i", std::cref(CdH_13i)));
483  ModelParamMap.insert(std::make_pair("CdH_22i", std::cref(CdH_22i)));
484  ModelParamMap.insert(std::make_pair("CdH_23i", std::cref(CdH_23i)));
485  ModelParamMap.insert(std::make_pair("CdH_33i", std::cref(CdH_33i)));
486  ModelParamMap.insert(std::make_pair("CuG_11r", std::cref(CuG_11r)));
487  ModelParamMap.insert(std::make_pair("CuG_12r", std::cref(CuG_12r)));
488  ModelParamMap.insert(std::make_pair("CuG_13r", std::cref(CuG_13r)));
489  ModelParamMap.insert(std::make_pair("CuG_22r", std::cref(CuG_22r)));
490  ModelParamMap.insert(std::make_pair("CuG_23r", std::cref(CuG_23r)));
491  ModelParamMap.insert(std::make_pair("CuG_33r", std::cref(CuG_33r)));
492  ModelParamMap.insert(std::make_pair("CuG_11i", std::cref(CuG_11i)));
493  ModelParamMap.insert(std::make_pair("CuG_12i", std::cref(CuG_12i)));
494  ModelParamMap.insert(std::make_pair("CuG_13i", std::cref(CuG_13i)));
495  ModelParamMap.insert(std::make_pair("CuG_22i", std::cref(CuG_22i)));
496  ModelParamMap.insert(std::make_pair("CuG_23i", std::cref(CuG_23i)));
497  ModelParamMap.insert(std::make_pair("CuG_33i", std::cref(CuG_33i)));
498  ModelParamMap.insert(std::make_pair("CuW_11r", std::cref(CuW_11r)));
499  ModelParamMap.insert(std::make_pair("CuW_12r", std::cref(CuW_12r)));
500  ModelParamMap.insert(std::make_pair("CuW_13r", std::cref(CuW_13r)));
501  ModelParamMap.insert(std::make_pair("CuW_22r", std::cref(CuW_22r)));
502  ModelParamMap.insert(std::make_pair("CuW_23r", std::cref(CuW_23r)));
503  ModelParamMap.insert(std::make_pair("CuW_33r", std::cref(CuW_33r)));
504  ModelParamMap.insert(std::make_pair("CuW_11i", std::cref(CuW_11i)));
505  ModelParamMap.insert(std::make_pair("CuW_12i", std::cref(CuW_12i)));
506  ModelParamMap.insert(std::make_pair("CuW_13i", std::cref(CuW_13i)));
507  ModelParamMap.insert(std::make_pair("CuW_22i", std::cref(CuW_22i)));
508  ModelParamMap.insert(std::make_pair("CuW_23i", std::cref(CuW_23i)));
509  ModelParamMap.insert(std::make_pair("CuW_33i", std::cref(CuW_33i)));
510  ModelParamMap.insert(std::make_pair("CuB_11r", std::cref(CuB_11r)));
511  ModelParamMap.insert(std::make_pair("CuB_12r", std::cref(CuB_12r)));
512  ModelParamMap.insert(std::make_pair("CuB_13r", std::cref(CuB_13r)));
513  ModelParamMap.insert(std::make_pair("CuB_22r", std::cref(CuB_22r)));
514  ModelParamMap.insert(std::make_pair("CuB_23r", std::cref(CuB_23r)));
515  ModelParamMap.insert(std::make_pair("CuB_33r", std::cref(CuB_33r)));
516  ModelParamMap.insert(std::make_pair("CuB_11i", std::cref(CuB_11i)));
517  ModelParamMap.insert(std::make_pair("CuB_12i", std::cref(CuB_12i)));
518  ModelParamMap.insert(std::make_pair("CuB_13i", std::cref(CuB_13i)));
519  ModelParamMap.insert(std::make_pair("CuB_22i", std::cref(CuB_22i)));
520  ModelParamMap.insert(std::make_pair("CuB_23i", std::cref(CuB_23i)));
521  ModelParamMap.insert(std::make_pair("CuB_33i", std::cref(CuB_33i)));
522  }
524  ModelParamMap.insert(std::make_pair("CLQ1", std::cref(CLQ1_1111)));
525  ModelParamMap.insert(std::make_pair("CLQ3", std::cref(CLQ3_1111)));
526  ModelParamMap.insert(std::make_pair("Ceu", std::cref(Ceu_1111)));
527  ModelParamMap.insert(std::make_pair("Ced", std::cref(Ced_1111)));
528  ModelParamMap.insert(std::make_pair("CLu", std::cref(CLu_1111)));
529  ModelParamMap.insert(std::make_pair("CLd", std::cref(CLd_1111)));
530  ModelParamMap.insert(std::make_pair("CQe", std::cref(CQe_1111)));
531  } else {
532  ModelParamMap.insert(std::make_pair("CLQ1_1111", std::cref(CLQ1_1111)));
533  ModelParamMap.insert(std::make_pair("CLQ1_1122", std::cref(CLQ1_1122)));
534  ModelParamMap.insert(std::make_pair("CLQ1_2211", std::cref(CLQ1_2211)));
535  ModelParamMap.insert(std::make_pair("CLQ1_1221", std::cref(CLQ1_1221)));
536  ModelParamMap.insert(std::make_pair("CLQ1_2112", std::cref(CLQ1_2112)));
537  ModelParamMap.insert(std::make_pair("CLQ1_1133", std::cref(CLQ1_1133)));
538  ModelParamMap.insert(std::make_pair("CLQ1_3311", std::cref(CLQ1_3311)));
539  ModelParamMap.insert(std::make_pair("CLQ1_1331", std::cref(CLQ1_1331)));
540  ModelParamMap.insert(std::make_pair("CLQ1_3113", std::cref(CLQ1_3113)));
541  ModelParamMap.insert(std::make_pair("CLQ1_1123", std::cref(CLQ1_1123)));
542  ModelParamMap.insert(std::make_pair("CLQ1_2223", std::cref(CLQ1_2223)));
543  ModelParamMap.insert(std::make_pair("CLQ1_3323", std::cref(CLQ1_3323)));
544  ModelParamMap.insert(std::make_pair("CLQ1_1132", std::cref(CLQ1_1132)));
545  ModelParamMap.insert(std::make_pair("CLQ1_2232", std::cref(CLQ1_2232)));
546  ModelParamMap.insert(std::make_pair("CLQ1_3332", std::cref(CLQ1_3332)));
547  ModelParamMap.insert(std::make_pair("CLQ3_1111", std::cref(CLQ3_1111)));
548  ModelParamMap.insert(std::make_pair("CLQ3_1122", std::cref(CLQ3_1122)));
549  ModelParamMap.insert(std::make_pair("CLQ3_2211", std::cref(CLQ3_2211)));
550  ModelParamMap.insert(std::make_pair("CLQ3_1221", std::cref(CLQ3_1221)));
551  ModelParamMap.insert(std::make_pair("CLQ3_2112", std::cref(CLQ3_2112)));
552  ModelParamMap.insert(std::make_pair("CLQ3_1133", std::cref(CLQ3_1133)));
553  ModelParamMap.insert(std::make_pair("CLQ3_3311", std::cref(CLQ3_3311)));
554  ModelParamMap.insert(std::make_pair("CLQ3_1331", std::cref(CLQ3_1331)));
555  ModelParamMap.insert(std::make_pair("CLQ3_3113", std::cref(CLQ3_3113)));
556  ModelParamMap.insert(std::make_pair("CLQ3_1123", std::cref(CLQ3_1123)));
557  ModelParamMap.insert(std::make_pair("CLQ3_2223", std::cref(CLQ3_2223)));
558  ModelParamMap.insert(std::make_pair("CLQ3_3323", std::cref(CLQ3_3323)));
559  ModelParamMap.insert(std::make_pair("CLQ3_1132", std::cref(CLQ3_1132)));
560  ModelParamMap.insert(std::make_pair("CLQ3_2232", std::cref(CLQ3_2232)));
561  ModelParamMap.insert(std::make_pair("CLQ3_3332", std::cref(CLQ3_3332)));
562  ModelParamMap.insert(std::make_pair("Ceu_1111", std::cref(Ceu_1111)));
563  ModelParamMap.insert(std::make_pair("Ceu_1122", std::cref(Ceu_1122)));
564  ModelParamMap.insert(std::make_pair("Ceu_2211", std::cref(Ceu_2211)));
565  ModelParamMap.insert(std::make_pair("Ceu_1133", std::cref(Ceu_1133)));
566  ModelParamMap.insert(std::make_pair("Ceu_2233", std::cref(Ceu_2233)));
567  ModelParamMap.insert(std::make_pair("Ceu_3311", std::cref(Ceu_3311)));
568  ModelParamMap.insert(std::make_pair("Ced_1111", std::cref(Ced_1111)));
569  ModelParamMap.insert(std::make_pair("Ced_1122", std::cref(Ced_1122)));
570  ModelParamMap.insert(std::make_pair("Ced_2211", std::cref(Ced_2211)));
571  ModelParamMap.insert(std::make_pair("Ced_1133", std::cref(Ced_1133)));
572  ModelParamMap.insert(std::make_pair("Ced_3311", std::cref(Ced_3311)));
573  ModelParamMap.insert(std::make_pair("Ced_1123", std::cref(Ced_1123)));
574  ModelParamMap.insert(std::make_pair("Ced_2223", std::cref(Ced_2223)));
575  ModelParamMap.insert(std::make_pair("Ced_3323", std::cref(Ced_3323)));
576  ModelParamMap.insert(std::make_pair("Ced_1132", std::cref(Ced_1132)));
577  ModelParamMap.insert(std::make_pair("Ced_2232", std::cref(Ced_2232)));
578  ModelParamMap.insert(std::make_pair("Ced_3332", std::cref(Ced_3332)));
579  ModelParamMap.insert(std::make_pair("CLu_1111", std::cref(CLu_1111)));
580  ModelParamMap.insert(std::make_pair("CLu_1122", std::cref(CLu_1122)));
581  ModelParamMap.insert(std::make_pair("CLu_2211", std::cref(CLu_2211)));
582  ModelParamMap.insert(std::make_pair("CLu_1133", std::cref(CLu_1133)));
583  ModelParamMap.insert(std::make_pair("CLu_2233", std::cref(CLu_2233)));
584  ModelParamMap.insert(std::make_pair("CLu_3311", std::cref(CLu_3311)));
585  ModelParamMap.insert(std::make_pair("CLd_1111", std::cref(CLd_1111)));
586  ModelParamMap.insert(std::make_pair("CLd_1122", std::cref(CLd_1122)));
587  ModelParamMap.insert(std::make_pair("CLd_2211", std::cref(CLd_2211)));
588  ModelParamMap.insert(std::make_pair("CLd_1133", std::cref(CLd_1133)));
589  ModelParamMap.insert(std::make_pair("CLd_3311", std::cref(CLd_3311)));
590  ModelParamMap.insert(std::make_pair("CLd_1123", std::cref(CLd_1123)));
591  ModelParamMap.insert(std::make_pair("CLd_2223", std::cref(CLd_2223)));
592  ModelParamMap.insert(std::make_pair("CLd_3323", std::cref(CLd_3323)));
593  ModelParamMap.insert(std::make_pair("CLd_1132", std::cref(CLd_1132)));
594  ModelParamMap.insert(std::make_pair("CLd_2232", std::cref(CLd_2232)));
595  ModelParamMap.insert(std::make_pair("CLd_3332", std::cref(CLd_3332)));
596  ModelParamMap.insert(std::make_pair("CQe_1111", std::cref(CQe_1111)));
597  ModelParamMap.insert(std::make_pair("CQe_1122", std::cref(CQe_1122)));
598  ModelParamMap.insert(std::make_pair("CQe_2211", std::cref(CQe_2211)));
599  ModelParamMap.insert(std::make_pair("CQe_1133", std::cref(CQe_1133)));
600  ModelParamMap.insert(std::make_pair("CQe_3311", std::cref(CQe_3311)));
601  ModelParamMap.insert(std::make_pair("CQe_2311", std::cref(CQe_2311)));
602  ModelParamMap.insert(std::make_pair("CQe_2322", std::cref(CQe_2322)));
603  ModelParamMap.insert(std::make_pair("CQe_2333", std::cref(CQe_2333)));
604  ModelParamMap.insert(std::make_pair("CQe_3211", std::cref(CQe_3211)));
605  ModelParamMap.insert(std::make_pair("CQe_3222", std::cref(CQe_3222)));
606  ModelParamMap.insert(std::make_pair("CQe_3233", std::cref(CQe_3233)));
607  ModelParamMap.insert(std::make_pair("CLedQ_11", std::cref(CLedQ_11)));
608  ModelParamMap.insert(std::make_pair("CLedQ_22", std::cref(CLedQ_22)));
609  ModelParamMap.insert(std::make_pair("CpLedQ_11", std::cref(CpLedQ_11)));
610  ModelParamMap.insert(std::make_pair("CpLedQ_22", std::cref(CpLedQ_22)));
611  }
612  ModelParamMap.insert(std::make_pair("Lambda_NP", std::cref(Lambda_NP)));
613  ModelParamMap.insert(std::make_pair("BrHinv", std::cref(BrHinv)));
614  ModelParamMap.insert(std::make_pair("BrHexo", std::cref(BrHexo)));
615  ModelParamMap.insert(std::make_pair("dg1Z", std::cref(dg1Z)));
616  ModelParamMap.insert(std::make_pair("dKappaga", std::cref(dKappaga)));
617  ModelParamMap.insert(std::make_pair("lambZ", std::cref(lambZ)));
618  ModelParamMap.insert(std::make_pair("eggFint", std::cref(eggFint)));
619  ModelParamMap.insert(std::make_pair("eggFpar", std::cref(eggFpar)));
620  ModelParamMap.insert(std::make_pair("ettHint", std::cref(ettHint)));
621  ModelParamMap.insert(std::make_pair("ettHpar", std::cref(ettHpar)));
622  ModelParamMap.insert(std::make_pair("eVBFint", std::cref(eVBFint)));
623  ModelParamMap.insert(std::make_pair("eVBFpar", std::cref(eVBFpar)));
624  ModelParamMap.insert(std::make_pair("eWHint", std::cref(eWHint)));
625  ModelParamMap.insert(std::make_pair("eWHpar", std::cref(eWHpar)));
626  ModelParamMap.insert(std::make_pair("eZHint", std::cref(eZHint)));
627  ModelParamMap.insert(std::make_pair("eZHpar", std::cref(eZHpar)));
628  ModelParamMap.insert(std::make_pair("eeeWBFint", std::cref(eeeWBFint)));
629  ModelParamMap.insert(std::make_pair("eeeWBFpar", std::cref(eeeWBFpar)));
630  ModelParamMap.insert(std::make_pair("eeeZHint", std::cref(eeeZHint)));
631  ModelParamMap.insert(std::make_pair("eeeZHpar", std::cref(eeeZHpar)));
632  ModelParamMap.insert(std::make_pair("eeettHint", std::cref(eeettHint)));
633  ModelParamMap.insert(std::make_pair("eeettHpar", std::cref(eeettHpar)));
634  ModelParamMap.insert(std::make_pair("eepWBFint", std::cref(eepWBFint)));
635  ModelParamMap.insert(std::make_pair("eepWBFpar", std::cref(eepWBFpar)));
636  ModelParamMap.insert(std::make_pair("eepZBFint", std::cref(eepZBFint)));
637  ModelParamMap.insert(std::make_pair("eepZBFpar", std::cref(eepZBFpar)));
638  ModelParamMap.insert(std::make_pair("eHggint", std::cref(eHggint)));
639  ModelParamMap.insert(std::make_pair("eHggpar", std::cref(eHggpar)));
640  ModelParamMap.insert(std::make_pair("eHWWint", std::cref(eHWWint)));
641  ModelParamMap.insert(std::make_pair("eHWWpar", std::cref(eHWWpar)));
642  ModelParamMap.insert(std::make_pair("eHZZint", std::cref(eHZZint)));
643  ModelParamMap.insert(std::make_pair("eHZZpar", std::cref(eHZZpar)));
644  ModelParamMap.insert(std::make_pair("eHZgaint", std::cref(eHZgaint)));
645  ModelParamMap.insert(std::make_pair("eHZgapar", std::cref(eHZgapar)));
646  ModelParamMap.insert(std::make_pair("eHgagaint", std::cref(eHgagaint)));
647  ModelParamMap.insert(std::make_pair("eHgagapar", std::cref(eHgagapar)));
648  ModelParamMap.insert(std::make_pair("eHmumuint", std::cref(eHmumuint)));
649  ModelParamMap.insert(std::make_pair("eHmumupar", std::cref(eHmumupar)));
650  ModelParamMap.insert(std::make_pair("eHtautauint", std::cref(eHtautauint)));
651  ModelParamMap.insert(std::make_pair("eHtautaupar", std::cref(eHtautaupar)));
652  ModelParamMap.insert(std::make_pair("eHccint", std::cref(eHccint)));
653  ModelParamMap.insert(std::make_pair("eHccpar", std::cref(eHccpar)));
654  ModelParamMap.insert(std::make_pair("eHbbint", std::cref(eHbbint)));
655  ModelParamMap.insert(std::make_pair("eHbbpar", std::cref(eHbbpar)));
656  ModelParamMap.insert(std::make_pair("eggFHgaga", std::cref(eggFHgaga)));
657  ModelParamMap.insert(std::make_pair("eggFHZga", std::cref(eggFHZga)));
658  ModelParamMap.insert(std::make_pair("eggFHZZ", std::cref(eggFHZZ)));
659  ModelParamMap.insert(std::make_pair("eggFHWW", std::cref(eggFHWW)));
660  ModelParamMap.insert(std::make_pair("eggFHtautau", std::cref(eggFHtautau)));
661  ModelParamMap.insert(std::make_pair("eggFHbb", std::cref(eggFHbb)));
662  ModelParamMap.insert(std::make_pair("eggFHmumu", std::cref(eggFHmumu)));
663  ModelParamMap.insert(std::make_pair("eVBFHgaga", std::cref(eVBFHgaga)));
664  ModelParamMap.insert(std::make_pair("eVBFHZga", std::cref(eVBFHZga)));
665  ModelParamMap.insert(std::make_pair("eVBFHZZ", std::cref(eVBFHZZ)));
666  ModelParamMap.insert(std::make_pair("eVBFHWW", std::cref(eVBFHWW)));
667  ModelParamMap.insert(std::make_pair("eVBFHtautau", std::cref(eVBFHtautau)));
668  ModelParamMap.insert(std::make_pair("eVBFHbb", std::cref(eVBFHbb)));
669  ModelParamMap.insert(std::make_pair("eVBFHmumu", std::cref(eVBFHmumu)));
670  ModelParamMap.insert(std::make_pair("eWHgaga", std::cref(eWHgaga)));
671  ModelParamMap.insert(std::make_pair("eWHZga", std::cref(eWHZga)));
672  ModelParamMap.insert(std::make_pair("eWHZZ", std::cref(eWHZZ)));
673  ModelParamMap.insert(std::make_pair("eWHWW", std::cref(eWHWW)));
674  ModelParamMap.insert(std::make_pair("eWHtautau", std::cref(eWHtautau)));
675  ModelParamMap.insert(std::make_pair("eWHbb", std::cref(eWHbb)));
676  ModelParamMap.insert(std::make_pair("eWHmumu", std::cref(eWHmumu)));
677  ModelParamMap.insert(std::make_pair("eZHgaga", std::cref(eZHgaga)));
678  ModelParamMap.insert(std::make_pair("eZHZga", std::cref(eZHZga)));
679  ModelParamMap.insert(std::make_pair("eZHZZ", std::cref(eZHZZ)));
680  ModelParamMap.insert(std::make_pair("eZHWW", std::cref(eZHWW)));
681  ModelParamMap.insert(std::make_pair("eZHtautau", std::cref(eZHtautau)));
682  ModelParamMap.insert(std::make_pair("eZHbb", std::cref(eZHbb)));
683  ModelParamMap.insert(std::make_pair("eZHmumu", std::cref(eZHmumu)));
684  ModelParamMap.insert(std::make_pair("ettHgaga", std::cref(ettHgaga)));
685  ModelParamMap.insert(std::make_pair("ettHZga", std::cref(ettHZga)));
686  ModelParamMap.insert(std::make_pair("ettHZZ", std::cref(ettHZZ)));
687  ModelParamMap.insert(std::make_pair("ettHWW", std::cref(ettHWW)));
688  ModelParamMap.insert(std::make_pair("ettHtautau", std::cref(ettHtautau)));
689  ModelParamMap.insert(std::make_pair("ettHbb", std::cref(ettHbb)));
690  ModelParamMap.insert(std::make_pair("ettHmumu", std::cref(ettHmumu)));
691  ModelParamMap.insert(std::make_pair("eVBFHinv", std::cref(eVBFHinv)));
692  ModelParamMap.insert(std::make_pair("eVHinv", std::cref(eVHinv)));
693  ModelParamMap.insert(std::make_pair("eVBF_2_Hbox", std::cref(eVBF_2_Hbox)));
694  ModelParamMap.insert(std::make_pair("eVBF_2_HQ1_11", std::cref(eVBF_2_HQ1_11)));
695  ModelParamMap.insert(std::make_pair("eVBF_2_Hu_11", std::cref(eVBF_2_Hu_11)));
696  ModelParamMap.insert(std::make_pair("eVBF_2_Hd_11", std::cref(eVBF_2_Hd_11)));
697  ModelParamMap.insert(std::make_pair("eVBF_2_HQ3_11", std::cref(eVBF_2_HQ3_11)));
698  ModelParamMap.insert(std::make_pair("eVBF_2_HD", std::cref(eVBF_2_HD)));
699  ModelParamMap.insert(std::make_pair("eVBF_2_HB", std::cref(eVBF_2_HB)));
700  ModelParamMap.insert(std::make_pair("eVBF_2_HW", std::cref(eVBF_2_HW)));
701  ModelParamMap.insert(std::make_pair("eVBF_2_HWB", std::cref(eVBF_2_HWB)));
702  ModelParamMap.insert(std::make_pair("eVBF_2_HG", std::cref(eVBF_2_HG)));
703  ModelParamMap.insert(std::make_pair("eVBF_2_DHB", std::cref(eVBF_2_DHB)));
704  ModelParamMap.insert(std::make_pair("eVBF_2_DHW", std::cref(eVBF_2_DHW)));
705  ModelParamMap.insert(std::make_pair("eVBF_2_DeltaGF", std::cref(eVBF_2_DeltaGF)));
706  ModelParamMap.insert(std::make_pair("eVBF_78_Hbox", std::cref(eVBF_78_Hbox)));
707  ModelParamMap.insert(std::make_pair("eVBF_78_HQ1_11", std::cref(eVBF_78_HQ1_11)));
708  ModelParamMap.insert(std::make_pair("eVBF_78_Hu_11", std::cref(eVBF_78_Hu_11)));
709  ModelParamMap.insert(std::make_pair("eVBF_78_Hd_11", std::cref(eVBF_78_Hd_11)));
710  ModelParamMap.insert(std::make_pair("eVBF_78_HQ3_11", std::cref(eVBF_78_HQ3_11)));
711  ModelParamMap.insert(std::make_pair("eVBF_78_HD", std::cref(eVBF_78_HD)));
712  ModelParamMap.insert(std::make_pair("eVBF_78_HB", std::cref(eVBF_78_HB)));
713  ModelParamMap.insert(std::make_pair("eVBF_78_HW", std::cref(eVBF_78_HW)));
714  ModelParamMap.insert(std::make_pair("eVBF_78_HWB", std::cref(eVBF_78_HWB)));
715  ModelParamMap.insert(std::make_pair("eVBF_78_HG", std::cref(eVBF_78_HG)));
716  ModelParamMap.insert(std::make_pair("eVBF_78_DHB", std::cref(eVBF_78_DHB)));
717  ModelParamMap.insert(std::make_pair("eVBF_78_DHW", std::cref(eVBF_78_DHW)));
718  ModelParamMap.insert(std::make_pair("eVBF_78_DeltaGF", std::cref(eVBF_78_DeltaGF)));
719  ModelParamMap.insert(std::make_pair("eVBF_1314_Hbox", std::cref(eVBF_1314_Hbox)));
720  ModelParamMap.insert(std::make_pair("eVBF_1314_HQ1_11", std::cref(eVBF_1314_HQ1_11)));
721  ModelParamMap.insert(std::make_pair("eVBF_1314_Hu_11", std::cref(eVBF_1314_Hu_11)));
722  ModelParamMap.insert(std::make_pair("eVBF_1314_Hd_11", std::cref(eVBF_1314_Hd_11)));
723  ModelParamMap.insert(std::make_pair("eVBF_1314_HQ3_11", std::cref(eVBF_1314_HQ3_11)));
724  ModelParamMap.insert(std::make_pair("eVBF_1314_HD", std::cref(eVBF_1314_HD)));
725  ModelParamMap.insert(std::make_pair("eVBF_1314_HB", std::cref(eVBF_1314_HB)));
726  ModelParamMap.insert(std::make_pair("eVBF_1314_HW", std::cref(eVBF_1314_HW)));
727  ModelParamMap.insert(std::make_pair("eVBF_1314_HWB", std::cref(eVBF_1314_HWB)));
728  ModelParamMap.insert(std::make_pair("eVBF_1314_HG", std::cref(eVBF_1314_HG)));
729  ModelParamMap.insert(std::make_pair("eVBF_1314_DHB", std::cref(eVBF_1314_DHB)));
730  ModelParamMap.insert(std::make_pair("eVBF_1314_DHW", std::cref(eVBF_1314_DHW)));
731  ModelParamMap.insert(std::make_pair("eVBF_1314_DeltaGF", std::cref(eVBF_1314_DeltaGF)));
732  ModelParamMap.insert(std::make_pair("eWH_2_Hbox", std::cref(eWH_2_Hbox)));
733  ModelParamMap.insert(std::make_pair("eWH_2_HQ3_11", std::cref(eWH_2_HQ3_11)));
734  ModelParamMap.insert(std::make_pair("eWH_2_HD", std::cref(eWH_2_HD)));
735  ModelParamMap.insert(std::make_pair("eWH_2_HW", std::cref(eWH_2_HW)));
736  ModelParamMap.insert(std::make_pair("eWH_2_HWB", std::cref(eWH_2_HWB)));
737  ModelParamMap.insert(std::make_pair("eWH_2_DHW", std::cref(eWH_2_DHW)));
738  ModelParamMap.insert(std::make_pair("eWH_2_DeltaGF", std::cref(eWH_2_DeltaGF)));
739  ModelParamMap.insert(std::make_pair("eWH_78_Hbox", std::cref(eWH_78_Hbox)));
740  ModelParamMap.insert(std::make_pair("eWH_78_HQ3_11", std::cref(eWH_78_HQ3_11)));
741  ModelParamMap.insert(std::make_pair("eWH_78_HD", std::cref(eWH_78_HD)));
742  ModelParamMap.insert(std::make_pair("eWH_78_HW", std::cref(eWH_78_HW)));
743  ModelParamMap.insert(std::make_pair("eWH_78_HWB", std::cref(eWH_78_HWB)));
744  ModelParamMap.insert(std::make_pair("eWH_78_DHW", std::cref(eWH_78_DHW)));
745  ModelParamMap.insert(std::make_pair("eWH_78_DeltaGF", std::cref(eWH_78_DeltaGF)));
746  ModelParamMap.insert(std::make_pair("eWH_1314_Hbox", std::cref(eWH_1314_Hbox)));
747  ModelParamMap.insert(std::make_pair("eWH_1314_HQ3_11", std::cref(eWH_1314_HQ3_11)));
748  ModelParamMap.insert(std::make_pair("eWH_1314_HD", std::cref(eWH_1314_HD)));
749  ModelParamMap.insert(std::make_pair("eWH_1314_HW", std::cref(eWH_1314_HW)));
750  ModelParamMap.insert(std::make_pair("eWH_1314_HWB", std::cref(eWH_1314_HWB)));
751  ModelParamMap.insert(std::make_pair("eWH_1314_DHW", std::cref(eWH_1314_DHW)));
752  ModelParamMap.insert(std::make_pair("eWH_1314_DeltaGF", std::cref(eWH_1314_DeltaGF)));
753  ModelParamMap.insert(std::make_pair("eZH_2_Hbox", std::cref(eZH_2_Hbox)));
754  ModelParamMap.insert(std::make_pair("eZH_2_HQ1_11", std::cref(eZH_2_HQ1_11)));
755  ModelParamMap.insert(std::make_pair("eZH_2_Hu_11", std::cref(eZH_2_Hu_11)));
756  ModelParamMap.insert(std::make_pair("eZH_2_Hd_11", std::cref(eZH_2_Hd_11)));
757  ModelParamMap.insert(std::make_pair("eZH_2_HQ3_11", std::cref(eZH_2_HQ3_11)));
758  ModelParamMap.insert(std::make_pair("eZH_2_HD", std::cref(eZH_2_HD)));
759  ModelParamMap.insert(std::make_pair("eZH_2_HB", std::cref(eZH_2_HB)));
760  ModelParamMap.insert(std::make_pair("eZH_2_HW", std::cref(eZH_2_HW)));
761  ModelParamMap.insert(std::make_pair("eZH_2_HWB", std::cref(eZH_2_HWB)));
762  ModelParamMap.insert(std::make_pair("eZH_2_DHB", std::cref(eZH_2_DHB)));
763  ModelParamMap.insert(std::make_pair("eZH_2_DHW", std::cref(eZH_2_DHW)));
764  ModelParamMap.insert(std::make_pair("eZH_2_DeltaGF", std::cref(eZH_2_DeltaGF)));
765  ModelParamMap.insert(std::make_pair("eZH_78_Hbox", std::cref(eZH_78_Hbox)));
766  ModelParamMap.insert(std::make_pair("eZH_78_HQ1_11", std::cref(eZH_78_HQ1_11)));
767  ModelParamMap.insert(std::make_pair("eZH_78_Hu_11", std::cref(eZH_78_Hu_11)));
768  ModelParamMap.insert(std::make_pair("eZH_78_Hd_11", std::cref(eZH_78_Hd_11)));
769  ModelParamMap.insert(std::make_pair("eZH_78_HQ3_11", std::cref(eZH_78_HQ3_11)));
770  ModelParamMap.insert(std::make_pair("eZH_78_HD", std::cref(eZH_78_HD)));
771  ModelParamMap.insert(std::make_pair("eZH_78_HB", std::cref(eZH_78_HB)));
772  ModelParamMap.insert(std::make_pair("eZH_78_HW", std::cref(eZH_78_HW)));
773  ModelParamMap.insert(std::make_pair("eZH_78_HWB", std::cref(eZH_78_HWB)));
774  ModelParamMap.insert(std::make_pair("eZH_78_DHB", std::cref(eZH_78_DHB)));
775  ModelParamMap.insert(std::make_pair("eZH_78_DHW", std::cref(eZH_78_DHW)));
776  ModelParamMap.insert(std::make_pair("eZH_78_DeltaGF", std::cref(eZH_78_DeltaGF)));
777  ModelParamMap.insert(std::make_pair("eZH_1314_Hbox", std::cref(eZH_1314_Hbox)));
778  ModelParamMap.insert(std::make_pair("eZH_1314_HQ1_11", std::cref(eZH_1314_HQ1_11)));
779  ModelParamMap.insert(std::make_pair("eZH_1314_Hu_11", std::cref(eZH_1314_Hu_11)));
780  ModelParamMap.insert(std::make_pair("eZH_1314_Hd_11", std::cref(eZH_1314_Hd_11)));
781  ModelParamMap.insert(std::make_pair("eZH_1314_HQ3_11", std::cref(eZH_1314_HQ3_11)));
782  ModelParamMap.insert(std::make_pair("eZH_1314_HD", std::cref(eZH_1314_HD)));
783  ModelParamMap.insert(std::make_pair("eZH_1314_HB", std::cref(eZH_1314_HB)));
784  ModelParamMap.insert(std::make_pair("eZH_1314_HW", std::cref(eZH_1314_HW)));
785  ModelParamMap.insert(std::make_pair("eZH_1314_HWB", std::cref(eZH_1314_HWB)));
786  ModelParamMap.insert(std::make_pair("eZH_1314_DHB", std::cref(eZH_1314_DHB)));
787  ModelParamMap.insert(std::make_pair("eZH_1314_DHW", std::cref(eZH_1314_DHW)));
788  ModelParamMap.insert(std::make_pair("eZH_1314_DeltaGF", std::cref(eZH_1314_DeltaGF)));
789  ModelParamMap.insert(std::make_pair("ettH_2_HG", std::cref(ettH_2_HG)));
790  ModelParamMap.insert(std::make_pair("ettH_2_G", std::cref(ettH_2_G)));
791  ModelParamMap.insert(std::make_pair("ettH_2_uG_33r", std::cref(ettH_2_uG_33r)));
792  ModelParamMap.insert(std::make_pair("ettH_2_DeltagHt", std::cref(ettH_2_DeltagHt)));
793  ModelParamMap.insert(std::make_pair("ettH_78_HG", std::cref(ettH_78_HG)));
794  ModelParamMap.insert(std::make_pair("ettH_78_G", std::cref(ettH_78_G)));
795  ModelParamMap.insert(std::make_pair("ettH_78_uG_33r", std::cref(ettH_78_uG_33r)));
796  ModelParamMap.insert(std::make_pair("ettH_78_DeltagHt", std::cref(ettH_78_DeltagHt)));
797  ModelParamMap.insert(std::make_pair("ettH_1314_HG", std::cref(ettH_1314_HG)));
798  ModelParamMap.insert(std::make_pair("ettH_1314_G", std::cref(ettH_1314_G)));
799  ModelParamMap.insert(std::make_pair("ettH_1314_uG_33r", std::cref(ettH_1314_uG_33r)));
800  ModelParamMap.insert(std::make_pair("ettH_1314_DeltagHt", std::cref(ettH_1314_DeltagHt)));
801 
802  if (FlagLeptonUniversal) {
803  CeH_12r = 0.0;
804  CeH_13r = 0.0;
805  CeH_23r = 0.0;
806  CeH_12i = 0.0;
807  CeH_13i = 0.0;
808  CeH_23i = 0.0;
809 
810 // bsll/sbll entries only interesting (for the moment) if non-lepton universal. Set to 0 otherwise
811  CLQ1_1123 = 0.0;
812  CLQ1_2223 = 0.0;
813  CLQ1_3323 = 0.0;
814  CLQ1_1132 = 0.0;
815  CLQ1_2232 = 0.0;
816  CLQ1_3332 = 0.0;
817 
818  CLQ3_1123 = 0.0;
819  CLQ3_2223 = 0.0;
820  CLQ3_3323 = 0.0;
821  CLQ3_1132 = 0.0;
822  CLQ3_2232 = 0.0;
823  CLQ3_3332 = 0.0;
824 
825  Ced_1123 = 0.0;
826  Ced_2223 = 0.0;
827  Ced_3323 = 0.0;
828  Ced_1132 = 0.0;
829  Ced_2232 = 0.0;
830  Ced_3332 = 0.0;
831 
832  CLd_1123 = 0.0;
833  CLd_2223 = 0.0;
834  CLd_3323 = 0.0;
835  CLd_1132 = 0.0;
836  CLd_2232 = 0.0;
837  CLd_3332 = 0.0;
838 
839  CQe_2311 = 0.0;
840  CQe_2322 = 0.0;
841  CQe_2333 = 0.0;
842  CQe_3211 = 0.0;
843  CQe_3222 = 0.0;
844  CQe_3233 = 0.0;
845  }
846  if (FlagQuarkUniversal) {
847  CuH_12r = 0.0;
848  CuH_13r = 0.0;
849  CuH_23r = 0.0;
850  CuH_12i = 0.0;
851  CuH_13i = 0.0;
852  CuH_23i = 0.0;
853 
854  CdH_12r = 0.0;
855  CdH_13r = 0.0;
856  CdH_23r = 0.0;
857  CdH_12i = 0.0;
858  CdH_13i = 0.0;
859  CdH_23i = 0.0;
860  }
861 }

Member Function Documentation

◆ AH_f()

gslpp::complex NPSMEFTd6::AH_f ( const double  tau) const

Fermionic loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings.

\(A^H_f(\tau)=2\tau [1+(1-\tau)f(\tau)]\)

Parameters
[in]

Definition at line 3271 of file NPSMEFTd6.cpp.

3272 {
3273  return (2.0 * tau * (1.0 + (1.0 - tau) * f_triangle(tau)));
3274 }

◆ AH_W()

gslpp::complex NPSMEFTd6::AH_W ( const double  tau) const

W loop function entering in the calculation of the effective \(H\gamma\gamma\) coupling.

\(A^H_W(\tau)=-[2+3\tau + 3\tau*(2-\tau) f(\tau)]\)

Parameters
[in]

Definition at line 3276 of file NPSMEFTd6.cpp.

3277 {
3278  return -( 2.0 + 3.0 * tau + 3.0 * tau * (2.0 - tau) * f_triangle(tau) );
3279 }

◆ AHZga_f()

gslpp::complex NPSMEFTd6::AHZga_f ( const double  tau,
const double  lambda 
) const

Fermionic loop function entering in the calculation of the effective \(HZ\gamma\) coupling.

Parameters
[in]

Definition at line 3281 of file NPSMEFTd6.cpp.

3282 {
3283  return I_triangle_1(tau,lambda) - I_triangle_2(tau,lambda);
3284 }

◆ AHZga_W()

gslpp::complex NPSMEFTd6::AHZga_W ( const double  tau,
const double  lambda 
) const

W loop function entering in the calculation of the effective \(HZ\gamma\) coupling.

Parameters
[in]

Definition at line 3286 of file NPSMEFTd6.cpp.

3287 {
3288  gslpp::complex tmp;
3289 
3290  double tan2w = trueSM.sW2() / trueSM.cW2();
3291 
3292  tmp = 4.0 * (3.0 - tan2w ) * I_triangle_2(tau,lambda);
3293 
3294  tmp = tmp + ((1.0 +2.0 / tau)* tan2w - (5.0 + 2.0/tau)) * I_triangle_1(tau,lambda);
3295 
3296  return sqrt(trueSM.cW2()) * tmp;
3297 }

◆ aPskPol()

double NPSMEFTd6::aPskPol ( const double  sqrt_s,
const double  Pol_em,
const double  Pol_ep 
) const
virtual

the angular parameter \(a\) from \(\mu_{e^+e^- \to ZH}\) (arXiv:1708.09079 [hep-ph]).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively
Returns
\(a_{eeZH}\)

Reimplemented from NPbase.

Definition at line 8615 of file NPSMEFTd6.cpp.

8616 {
8617 
8618  // Expression missing CLL contributions!
8619 
8620  double aL, aR, aPol;
8621  double sM = sqrt_s * sqrt_s;
8622  double Mz2 = Mz*Mz;
8623  double MH2 = mHl*mHl;
8624  double dMz = 0.0;
8625  double dMH = 0.0;
8626  double dv,dg,dgp,dgL,dgR;
8627  double kCM, kCM2, EZ, EZ2, kZ, kH;
8628  double EtaZ;
8629  double CHpsk, CTpsk,CHL,CHLp, CHE;
8630  double CWB, CBB, CWW;
8631 
8632  // Convention for dim 6 operators
8634  CBB = 0.25 * (g2_tree*g2_tree/g1_tree/g1_tree) * CiHB * v2_over_LambdaNP2;
8635  CWW = 0.25 * CiHW * v2_over_LambdaNP2;
8636 
8637  CHpsk = ( -2.0 * CiHbox + 0.25 * CiHD ) * v2_over_LambdaNP2;
8638  CTpsk = -0.5 * CiHD * v2_over_LambdaNP2;
8639  CHL = CiHL1_11 * v2_over_LambdaNP2;
8640  CHLp = CiHL3_11 * v2_over_LambdaNP2;
8641  CHE = CiHe_11 * v2_over_LambdaNP2;
8642 
8643  // Other parameters (1): Missing CLL!!!
8644  dv = 0.5 * ( CiHL3_11 + CiHL3_22 )* v2_over_LambdaNP2;
8645 
8646  // WFR
8647  EtaZ = -(1.0/2.0)*CHpsk + 2.0*dMz - dv - CTpsk;
8648 
8649  // Kinematics
8650  kCM = sqrt( (sM*sM + (MH2 - Mz2)*(MH2 - Mz2) - 2.0*sM*(MH2 + Mz2))/(4.0*sM) );
8651  kCM2 = kCM*kCM;
8652 
8653  EZ = sqrt( Mz2 + kCM2);
8654  EZ2 = EZ*EZ;
8655 
8656  kZ = 2.0*Mz2/(sM - Mz2) + (EZ*Mz2)/(2*kCM2*sqrt_s) - Mz2/(2*kCM2) - (EZ2/Mz2)/(2.0 + EZ2/Mz2)*(1.0 - Mz2/(EZ*sqrt_s));
8657 
8658  kH = -((EZ*MH2)/(2*kCM2*sqrt_s)) - (EZ2/Mz2)/(2 + EZ2/Mz2)*MH2/(EZ*sqrt_s);
8659 
8660  // Other parameters (2): Missing CLL!!!
8661  dg = -(1.0/(g1_tree * ( cW2_tree*cW2_tree - sW2_tree*sW2_tree))) * ( dv * cW2_tree * g1_tree
8662  - cW2_tree * dMz * g1_tree + 0.25 * CiHD * cW2_tree * g1_tree * v2_over_LambdaNP2
8665 
8666 
8667  dgp = -(1.0/(cW2_tree * g1_tree * g1_tree * (-cW2_tree*cW2_tree + sW2_tree*sW2_tree))) * ( dv * cW2_tree * g1_tree * g1_tree * sW2_tree
8673 
8674  dgL = (1.0/(0.5 - sW2_tree))*(cW2_tree*(0.5 + sW2_tree)*dg
8675  - sW2_tree*(0.5 + cW2_tree)*dgp
8676  + 0.5*(CHL + CHLp)
8677  + 0.25*cW2_tree*(1.0 + 2.0*sW2_tree)*8.0*CWW
8678  - 0.5*sW2_tree*(1.0 - 2.0*sW2_tree)*8.0*CWB
8679  - 0.25*sW2_tree*sW2_tree/cW2_tree*(1.0 + 2.0*cW2_tree)*8.0*CBB);
8680 
8681  dgR = -cW2_tree*dg + (1.0 + cW2_tree)*dgp
8682  - 1.0/(2.0*sW2_tree)*CHE - 0.5*cW2_tree*8*CWW
8683  + cW2_tree*8.0*CWB + 0.5*sW2_tree/cW2_tree*(1.0 + cW2_tree)*8.0*CBB;
8684 
8685 
8686  // LH and RH pars
8687 
8688  aL = dgL + 2*dMz - dv + EtaZ + (sM - Mz2)/(2*Mz2)*(CHL + CHLp)/(0.5 - sW2_tree) + kZ*dMz + kH*dMH;
8689  aR = dgR + 2*dMz - dv + EtaZ - (sM - Mz2)/(2*Mz2)*CHE/sW2_tree + kZ*dMz + kH*dMH;
8690 
8691  // Polarized a parameter
8692  aPol = 0.25 * ( (1.0 - Pol_em/100.0)*(1.0 + Pol_ep/100.0) * aL
8693  + (1.0 + Pol_em/100.0)*(1.0 - Pol_ep/100.0) * aR );
8694 
8695  return aPol;
8696 }

◆ AuxObs_NP1()

double NPSMEFTd6::AuxObs_NP1 ( ) const
virtual

Auxiliary observable AuxObs_NP1 (See code for details.)

Returns
AuxObs_NP1

Reimplemented from NPbase.

Definition at line 15295 of file NPSMEFTd6.cpp.

15296 {
15297  // To be used for some temporary observable
15298 
15299  // WY analysis at 13 TeV for HL-LHC 3/ab
15300  double Wpar, Ypar, Wpar2, Ypar2;
15301  double Chi2NC13, Chi2CC13, Chi2Tot;
15302 
15303  Wpar = 10000.0 * obliqueW();
15304  Ypar = 10000.0 * obliqueY();
15305 
15306  Wpar2 = Wpar*Wpar;
15307  Ypar2 = Ypar*Ypar;
15308 
15309  Chi2CC13 = Wpar2 * (18.365037149441695 + 2.422904241798858 * Wpar + 0.12120594308623695 * Wpar2);
15310 
15311  Chi2NC13 = 0.032772034538390675 * Wpar2*Wpar2 + 2.815243944990361 * Ypar2 - 0.36522061776278516 * Ypar2*Ypar
15312  + 0.017375258924241194 * Ypar2*Ypar2 + Wpar2*Wpar * (-0.7059117582389635 + 0.006816297425306027 * Ypar)
15313  + Wpar * Ypar * (7.988302197022343 + Ypar * (-0.5450119819316416 + 0.0050292149953719766 * Ypar))
15314  + Wpar2 * (5.68581760491364 + Ypar * (-0.5794111075840261 + 0.048026245835369625 * Ypar));
15315 
15316  Chi2Tot = Chi2CC13 + Chi2NC13;
15317 
15318  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
15319  return sqrt(Chi2Tot);
15320 }

◆ AuxObs_NP10()

double NPSMEFTd6::AuxObs_NP10 ( ) const
virtual

Auxiliary observable AuxObs_NP10 (See code for details.)

Returns
AuxObs_NP10

Reimplemented from NPbase.

Definition at line 15896 of file NPSMEFTd6.cpp.

15897 {
15898  // CLIC STWY using difermion production at all energies: 380 and 1500 GeV
15899  double Spar, Tpar, Wpar, Ypar, Spar2, Tpar2, Wpar2, Ypar2;
15900  double Chi2Tot;
15901 
15902  Spar = obliqueS();
15903  Tpar = obliqueT();
15904  Wpar = 10000.0 * obliqueW();
15905  Ypar = 10000.0 * obliqueY();
15906 
15907  Spar2 = Spar*Spar;
15908  Tpar2 = Tpar*Tpar;
15909  Wpar2 = Wpar*Wpar;
15910  Ypar2 = Ypar*Ypar;
15911 
15912  Chi2Tot = 375.63808963031073 * Spar2
15913  - 617.8864704052573 * Spar * Tpar
15914  + 353.1650032169891 * Tpar2
15915  + 215.96605851087603 * Spar * Wpar
15916  - 309.3469843690006 * Tpar * Wpar
15917  + 518.10263970583244 * Wpar2
15918  - 45.972763923203014 * Spar * Ypar
15919  - 40.670385844305705 * Tpar * Ypar
15920  + 340.56677318671185 * Wpar * Ypar
15921  + 364.5290176991845 * Ypar2;
15922 
15923  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
15924  return sqrt(Chi2Tot);
15925 }

◆ AuxObs_NP11()

double NPSMEFTd6::AuxObs_NP11 ( ) const
virtual

Auxiliary observable AuxObs_NP11 (See code for details.)

Returns
AuxObs_NP11

Reimplemented from NPbase.

Definition at line 15927 of file NPSMEFTd6.cpp.

15928 {
15929  // CLIC STWY using difermion production at all energies: 380 GeV
15930  double Spar, Tpar, Wpar, Ypar, Spar2, Tpar2, Wpar2, Ypar2;
15931  double Chi2Tot;
15932 
15933  Spar = obliqueS();
15934  Tpar = obliqueT();
15935  Wpar = 10000.0 * obliqueW();
15936  Ypar = 10000.0 * obliqueY();
15937 
15938  Spar2 = Spar*Spar;
15939  Tpar2 = Tpar*Tpar;
15940  Wpar2 = Wpar*Wpar;
15941  Ypar2 = Ypar*Ypar;
15942 
15943  Chi2Tot = 282.9842573293628 * Spar2
15944  - 462.32090035841725 * Spar * Tpar
15945  + 276.2496928300019 * Tpar2
15946  + 66.08702076419566 * Spar * Wpar
15947  - 87.95794393624075 * Tpar * Wpar
15948  + 9.5435699879102 * Wpar2
15949  - 26.170009941328716 * Spar * Ypar
15950  - 9.695238064023518 * Tpar * Ypar
15951  + 6.519573295893438 * Wpar * Ypar
15952  + 12.858593910798793 * Ypar2;
15953 
15954  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
15955  return sqrt(Chi2Tot);
15956 }

◆ AuxObs_NP12()

double NPSMEFTd6::AuxObs_NP12 ( ) const
virtual

Auxiliary observable AuxObs_NP12 (See code for details.)

Returns
AuxObs_NP12

Reimplemented from NPbase.

Definition at line 15958 of file NPSMEFTd6.cpp.

15959 {
15960  // CLIC dim6 Top fit 1500 GeV: only for SVF operators
15961  double CHqminus, CHt;
15962  double Chi2Tot;
15963 
15964  // The chi2 is given assuming C/Lambda^2 is in units of TeV^-2
15965  CHqminus= 0.5 * (CiHQ1_33 - CiHQ3_33) * (1000000.0 / LambdaNP2);
15966  CHt= 0.5 * CiHu_33 * (1000000.0 / LambdaNP2);
15967 
15968  Chi2Tot= 1203.58 * CHqminus * CHqminus + 1661.59 * CHqminus * CHt + 1257.83 * CHt * CHt;
15969 
15970  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
15971  return sqrt(Chi2Tot);
15972 }

◆ AuxObs_NP13()

double NPSMEFTd6::AuxObs_NP13 ( ) const
virtual

Auxiliary observable AuxObs_NP13.

Returns
AuxObs_NP13

Reimplemented from NPbase.

Definition at line 15974 of file NPSMEFTd6.cpp.

15975 {
15976  // CLIC dim6 Top fit 3000 GeV: only for SVF operators
15977  double CHqminus, CHt;
15978  double Chi2Tot;
15979 
15980  // The chi2 is given assuming C/Lambda^2 is in units of TeV^-2
15981  CHqminus= 0.5 * (CiHQ1_33 - CiHQ3_33) * (1000000.0 / LambdaNP2);
15982  CHt= 0.5 * CiHu_33 * (1000000.0 / LambdaNP2);
15983 
15984  Chi2Tot= 5756.01 * CHqminus * CHqminus + 8013.79 * CHqminus * CHt + 3380.7 * CHt * CHt;
15985 
15986  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
15987  return sqrt(Chi2Tot);
15988 }

◆ AuxObs_NP14()

double NPSMEFTd6::AuxObs_NP14 ( ) const
virtual

Auxiliary observable AuxObs_NP14.

Returns
AuxObs_NP14

Reimplemented from NPbase.

Definition at line 15990 of file NPSMEFTd6.cpp.

15991 {
15992  // Test chi2 for HH production at 100 TeV: only the first two bins in 1704.01953 are included,
15993  // with the same coefficients (including ratios of cross sections in each bin) its table 4. The EFT parameterization of Higgs decays are not included.
15994  double Chi2Tot;
15995 
15996 // Higgs basis parameters
15997  double dcZHB,cggHB;
15998  double dytHB;
15999  double dKlambda;
16000 
16001  dcZHB = deltacZ_HB();
16002  cggHB = cgg_HB();
16003  dytHB = deltayt_HB();
16004  dKlambda = deltaG_hhhRatio();
16005 
16006  double dcZHB2,dcZHB3,dcZHB4;
16007  double cggHB2,cggHB3,cggHB4;
16008  double dytHB2,dytHB3,dytHB4,dytHB5,dytHB6,dytHB7,dytHB8;
16009  double dKlambda2,dKlambda3,dKlambda4;
16010 
16011  dcZHB2 = dcZHB * dcZHB;
16012  dcZHB3 = dcZHB2 * dcZHB;
16013  dcZHB4 = dcZHB3 * dcZHB;
16014 
16015  cggHB2 = cggHB * cggHB;
16016  cggHB3 = cggHB2 * cggHB;
16017  cggHB4 = cggHB3 * cggHB;
16018 
16019  dytHB2 = dytHB * dytHB;
16020  dytHB3 = dytHB2 * dytHB;
16021  dytHB4 = dytHB3 * dytHB;
16022  dytHB5 = dytHB4 * dytHB;
16023  dytHB6 = dytHB5 * dytHB;
16024  dytHB7 = dytHB6 * dytHB;
16025  dytHB8 = dytHB7 * dytHB;
16026 
16027  dKlambda2 = dKlambda * dKlambda;
16028  dKlambda3 = dKlambda2 * dKlambda;
16029  dKlambda4 = dKlambda3 * dKlambda;
16030 
16031  // The Chi2
16032 
16033  Chi2Tot = 2.0595082782796297e7 * cggHB2 - 3.6971136499764752e9 * cggHB3 + 1.7583900534677216e11 * cggHB4
16034  - 630035.4483047676 * cggHB * dcZHB + 1.3588174266991532e8 * cggHB2 * dcZHB - 7.10364464231958e9 * cggHB3 * dcZHB
16035  + 5311.651853836387 * dcZHB2 - 1.7067170379207395e6 * cggHB * dcZHB2 + 1.1851653627034137e8 * cggHB2 * dcZHB2
16036  + 8180.119549200313 * dcZHB3 - 943018.2335425722 * cggHB * dcZHB3 + 3159.9135213745994 * dcZHB4
16037  + 180518.97210352542 * cggHB * dKlambda - 2.8949546963646576e7 * cggHB2 * dKlambda - 5.501576225306801e8 * cggHB3 * dKlambda
16038  + 1.5079027448500854e11 * cggHB4 * dKlambda - 2846.9365320948145 * dcZHB * dKlambda + 797208.485191074 * cggHB * dcZHB * dKlambda
16039  - 4.978486710457227e6 * cggHB2 * dcZHB * dKlambda - 4.586348042437428e9 * cggHB3 * dcZHB * dKlambda - 6485.875373880575 * dcZHB2 * dKlambda
16040  + 390177.86145601963 * cggHB * dcZHB2 * dKlambda + 5.056678567468029e7 * cggHB2 * dcZHB2 * dKlambda - 3291.6842405815532 * dcZHB3 * dKlambda
16041  - 198301.99217208195 * cggHB * dcZHB3 * dKlambda + 399.29685823653153 * dKlambda2 - 95580.41780509672 * cggHB * dKlambda2
16042  - 7.430874086734321e6 * cggHB2 * dKlambda2 + 7.720064658809748e8 * cggHB3 * dKlambda2 + 5.089872992160051e10 * cggHB4 * dKlambda2
16043  + 1809.9095844013955 * dcZHB * dKlambda2 - 1150.4119995786175 * cggHB * dcZHB * dKlambda2 - 2.2786176268418655e7 * cggHB2 * dcZHB * dKlambda2
16044  - 1.0351049455121036e9 * cggHB3 * dcZHB * dKlambda2 + 1362.5781363223641 * dcZHB2 * dKlambda2 + 170792.06609378837 * cggHB * dcZHB2 * dKlambda2
16045  + 5.658917948194164e6 * cggHB2 * dcZHB2 * dKlambda2 - 178.77181321253659 * dKlambda3 - 11443.938844928987 * cggHB * dKlambda3
16046  + 2.461878722072089e6 * cggHB2 * dKlambda3 + 2.821167791764089e8 * cggHB3 * dKlambda3 + 7.998289700049803e9 * cggHB4 * dKlambda3
16047  - 267.7615464146533 * dcZHB * dKlambda3 - 52488.33374581051 * cggHB * dcZHB * dKlambda3 - 3.555711022595523e6 * cggHB2 * dcZHB * dKlambda3
16048  - 8.149153208622633e7 * cggHB3 * dcZHB * dKlambda3 + 21.07398490236267 * dKlambda4 + 5735.3996792942135 * cggHB * dKlambda4
16049  + 596986.3215027236 * cggHB2 * dKlambda4 + 2.773647081412465e7 * cggHB3 * dKlambda4 + 4.915460918180312e8 * cggHB4 * dKlambda4
16050  + 740876.8879497008 * cggHB * dytHB - 1.938279550686329e8 * cggHB2 * dytHB + 1.1944585224312653e10 * cggHB3 * dytHB
16051  - 12947.635844899749 * dcZHB * dytHB + 4.908519506685015e6 * cggHB * dcZHB * dytHB - 3.742271337006843e8 * cggHB2 * dcZHB * dytHB
16052  - 33546.241370498166 * dcZHB2 * dytHB + 4.3134482870087875e6 * cggHB * dcZHB2 * dytHB - 18267.038917513022 * dcZHB3 * dytHB
16053  + 3387.385955080094 * dKlambda * dytHB - 963072.1570381082 * cggHB * dKlambda * dytHB - 2.3453010760683898e7 * cggHB2 * dKlambda * dytHB
16054  + 9.317798790237669e9 * cggHB3 * dKlambda * dytHB + 14461.190498065112 * dcZHB * dKlambda * dytHB - 276210.0620250288 * cggHB * dcZHB * dKlambda * dytHB
16055  - 2.1850896154428744e8 * cggHB2 * dcZHB * dKlambda * dytHB + 7442.375770947524 * dcZHB2 * dKlambda * dytHB
16056  + 1.6339998473341048e6 * cggHB * dcZHB2 * dKlambda * dytHB - 3291.6842405815532 * dcZHB3 * dKlambda * dytHB - 1559.6600507789517 * dKlambda2 * dytHB
16057  - 212800.20942464058 * cggHB * dKlambda2 * dytHB + 3.499621075016396e7 * cggHB2 * dKlambda2 * dytHB + 2.9495867407085886e9 * cggHB3 * dKlambda2 * dytHB
16058  - 132.54584108464164 * dcZHB * dKlambda2 * dytHB - 704650.5551856682 * cggHB * dcZHB * dKlambda2 * dytHB
16059  - 4.6230021860231325e7 * cggHB2 * dcZHB * dKlambda2 * dytHB + 2725.1562726447282 * dcZHB2 * dKlambda2 * dytHB
16060  + 170792.06609378837 * cggHB * dcZHB2 * dKlambda2 * dytHB - 174.87036642817392 * dKlambda3 * dytHB + 72002.66692264378 * cggHB * dKlambda3 * dytHB
16061  + 1.2160354917437742e7 * cggHB2 * dKlambda3 * dytHB + 4.500393455278235e8 * cggHB3 * dKlambda3 * dytHB - 803.2846392439599 * dcZHB * dKlambda3 * dytHB
16062  - 104976.66749162102 * cggHB * dcZHB * dKlambda3 * dytHB - 3.555711022595523e6 * cggHB2 * dcZHB * dKlambda3 * dytHB
16063  + 84.29593960945068 * dKlambda4 * dytHB + 17206.19903788264 * cggHB * dKlambda4 * dytHB + 1.1939726430054472e6 * cggHB2 * dKlambda4 * dytHB
16064  + 2.773647081412465e7 * cggHB3 * dKlambda4 * dytHB + 7985.615632692477 * dytHB2 - 4.312707242837639e6 * cggHB * dytHB2
16065  + 4.446488644358661e8 * cggHB2 * dytHB2 - 5.669235052669609e9 * cggHB3 * dytHB2 + 59322.05816648064 * dcZHB * dytHB2
16066  - 1.0048203483978426e7 * cggHB * dcZHB * dytHB2 + 2.009903412514487e8 * cggHB2 * dcZHB * dytHB2 + 64971.66315898899 * dcZHB2 * dytHB2
16067  - 2.4669987769536236e6 * cggHB * dcZHB2 * dytHB2 + 11471.803789781865 * dcZHB3 * dytHB2 - 11811.249755773804 * dKlambda * dytHB2
16068  + 431747.7364057698 * cggHB * dKlambda * dytHB2 + 2.2358583287946397e8 * cggHB2 * dKlambda * dytHB2 - 3.8910877145439386e9 * cggHB3 * dKlambda * dytHB2
16069  - 16029.606555240167 * dcZHB * dKlambda * dytHB2 - 2.9253661324121524e6 * cggHB * dcZHB * dKlambda * dytHB2
16070  + 8.987023921425158e7 * cggHB2 * dcZHB * dKlambda * dytHB2 + 4717.219498302798 * dcZHB2 * dKlambda * dytHB2
16071  - 540895.9436706528 * cggHB * dcZHB2 * dKlambda * dytHB2 + 214.81067429237223 * dKlambda2 * dytHB2 + 567954.341114266 * cggHB * dKlambda2 * dytHB2
16072  + 4.5123619667514816e7 * cggHB2 * dKlambda2 * dytHB2 - 9.277345617086976e8 * cggHB3 * dKlambda2 * dytHB2
16073  - 3081.626211728115 * dcZHB * dKlambda2 * dytHB2 - 381097.4778098703 * cggHB * dcZHB * dKlambda2 * dytHB2
16074  + 1.050966209735231e7 * cggHB2 * dcZHB * dKlambda2 * dytHB2 + 1362.5781363223641 * dcZHB2 * dKlambda2 * dytHB2
16075  + 284.9520271687106 * dKlambda3 * dytHB2 + 127206.63260007375 * cggHB * dKlambda3 * dytHB2 + 6.267940600872645e6 * cggHB2 * dKlambda3 * dytHB2
16076  - 7.655202990726441e7 * cggHB3 * dKlambda3 * dytHB2 - 803.2846392439599 * dcZHB * dKlambda3 * dytHB2 - 52488.33374581051 * cggHB * dcZHB * dKlambda3 * dytHB2
16077  + 126.44390941417602 * dKlambda4 * dytHB2 + 17206.19903788264 * cggHB * dKlambda4 * dytHB2 + 596986.3215027236 * cggHB2 * dKlambda4 * dytHB2
16078  - 37223.626257417236 * dytHB3 + 8.269994128894571e6 * cggHB * dytHB3 - 2.9221928856272686e8 * cggHB2 * dytHB3 - 105038.22976459829 * dcZHB * dytHB3
16079  + 7.149383019204844e6 * cggHB * dcZHB * dytHB3 - 47474.492515326274 * dcZHB2 * dytHB3 + 11656.27418420629 * dKlambda * dytHB3
16080  + 2.385352845620739e6 * cggHB * dKlambda * dytHB3 - 1.8438201632292444e8 * cggHB2 * dKlambda * dytHB3 - 8524.8765354653 * dcZHB * dKlambda * dytHB3
16081  + 2.8867300035650665e6 * cggHB * dcZHB * dKlambda * dytHB3 - 9211.031646525304 * dcZHB2 * dKlambda * dytHB3 + 3263.1999469874036 * dKlambda2 * dytHB3
16082  + 44138.45406924717 * cggHB * dKlambda2 * dytHB3 - 4.193837918690795e7 * cggHB2 * dKlambda2 * dytHB3 + 1474.023437403278 * dcZHB * dKlambda2 * dytHB3
16083  + 322402.6653762193 * cggHB * dcZHB * dKlambda2 * dytHB3 + 116.36014794980927 * dKlambda3 * dytHB3 - 7370.4909474997985 * cggHB * dKlambda3 * dytHB3
16084  - 3.4305355944930054e6 * cggHB2 * dKlambda3 * dytHB3 - 267.7615464146533 * dcZHB * dKlambda3 * dytHB3 + 84.29593960945068 * dKlambda4 * dytHB3
16085  + 5735.3996792942135 * cggHB * dKlambda4 * dytHB3 + 66652.27308402126 * dytHB4 - 6.871040436399154e6 * cggHB * dytHB4
16086  + 9.22099747455498e7 * cggHB2 * dytHB4 + 92021.78032189047 * dcZHB * dytHB4 - 2.257899878309953e6 * cggHB * dcZHB * dytHB4
16087  + 16245.693309808961 * dcZHB2 * dytHB4 + 2838.4331580144003 * dKlambda * dytHB4 - 2.731422853592693e6 * cggHB * dKlambda * dytHB4
16088  + 4.274439860749665e7 * cggHB2 * dKlambda * dytHB4 + 15892.926730807862 * dcZHB * dKlambda * dytHB4 - 515009.5486394962 * cggHB * dcZHB * dKlambda * dytHB4
16089  - 1056.6073875703482 * dKlambda2 * dytHB4 - 482475.3464808796 * cggHB * dKlambda2 * dytHB4 + 5.170468004804585e6 * cggHB2 * dKlambda2 * dytHB4
16090  + 2613.194223645355 * dcZHB * dKlambda2 * dytHB4 - 427.75818525652596 * dKlambda3 * dytHB4 - 51130.51778000078 * cggHB * dKlambda3 * dytHB4
16091  + 21.07398490236267 * dKlambda4 * dytHB4 - 63203.969008703876 * dytHB5 + 3.151938475204292e6 * cggHB * dytHB5 - 42834.09620756765 * dcZHB * dytHB5
16092  - 12524.979109927113 * dKlambda * dytHB5 + 1.3421161655790398e6 * cggHB * dKlambda * dytHB5 - 8919.930319126936 * dcZHB * dKlambda * dytHB5
16093  - 849.49051561947 * dKlambda2 * dytHB5 + 158560.3321836832 * cggHB * dKlambda2 * dytHB5 - 263.0677528219873 * dKlambda3 * dytHB5
16094  + 37913.4502786983 * dytHB6 - 712582.2268647491 * cggHB * dytHB6 + 10593.332328402174 * dcZHB * dytHB6 + 8514.598993531516 * dKlambda * dytHB6
16095  - 169200.83566434312 * cggHB * dKlambda * dytHB6 + 1296.5492356304262 * dKlambda2 * dytHB6 - 13281.426292006341 * dytHB7
16096  - 2976.898633587163 * dKlambda * dytHB7 + 2684.433665848417 * dytHB8;
16097 
16098  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
16099  return sqrt(Chi2Tot);
16100 }

◆ AuxObs_NP15()

double NPSMEFTd6::AuxObs_NP15 ( ) const
virtual

Auxiliary observable AuxObs_NP15.

Returns
AuxObs_NP15

Reimplemented from NPbase.

Definition at line 16102 of file NPSMEFTd6.cpp.

16103 {
16104  // To be used for some temporary observable
16105  return 0.0;
16106 }

◆ AuxObs_NP16()

double NPSMEFTd6::AuxObs_NP16 ( ) const
virtual

Auxiliary observable AuxObs_NP16.

Returns
AuxObs_NP16

Reimplemented from NPbase.

Definition at line 16108 of file NPSMEFTd6.cpp.

16109 {
16110  // To be used for some temporary observable
16111  return 0.0;
16112 }

◆ AuxObs_NP17()

double NPSMEFTd6::AuxObs_NP17 ( ) const
virtual

Auxiliary observable AuxObs_NP17.

Returns
AuxObs_NP17

Reimplemented from NPbase.

Definition at line 16114 of file NPSMEFTd6.cpp.

16115 {
16116  // To be used for some temporary observable
16117  return 0.0;
16118 }

◆ AuxObs_NP18()

double NPSMEFTd6::AuxObs_NP18 ( ) const
virtual

Auxiliary observable AuxObs_NP18.

Returns
AuxObs_NP18

Reimplemented from NPbase.

Definition at line 16120 of file NPSMEFTd6.cpp.

16121 {
16122  // To be used for some temporary observable
16123  return 0.0;
16124 }

◆ AuxObs_NP19()

double NPSMEFTd6::AuxObs_NP19 ( ) const
virtual

Auxiliary observable AuxObs_NP19.

Returns
AuxObs_NP19

Reimplemented from NPbase.

Definition at line 16126 of file NPSMEFTd6.cpp.

16127 {
16128  // To be used for some temporary observable
16129  return 0.0;
16130 }

◆ AuxObs_NP2()

double NPSMEFTd6::AuxObs_NP2 ( ) const
virtual

Auxiliary observable AuxObs_NP2 (See code for details.)

Returns
AuxObs_NP2

Reimplemented from NPbase.

Definition at line 15322 of file NPSMEFTd6.cpp.

15323 {
15324  // To be used for some temporary observable
15325 
15326  // WY analysis at 13 TeV for HL-LHC 3/ab for the CC
15327  // WY analysis at 27 TeV for HE-LHC 15/ab for the NC. 5% systematics (corr and uncorr)
15328  double Wpar, Ypar, Wpar2, Ypar2;
15329  double Chi2NC27, Chi2CC13, Chi2Tot;
15330 
15331  Wpar = 10000.0 * obliqueW();
15332  Ypar = 10000.0 * obliqueY();
15333 
15334  Wpar2 = Wpar*Wpar;
15335  Ypar2 = Ypar*Ypar;
15336 
15337  Chi2CC13 = Wpar2 * (18.365037149441695 + 2.422904241798858 * Wpar + 0.12120594308623695 * Wpar2);
15338 
15339  Chi2NC27 = 21.139285368181907 * Wpar2*Wpar2 + Wpar2*Wpar * (-89.16828370317616 + 7.182929295852857 * Ypar)
15340  + Wpar * Ypar * (208.8092257396059 + Ypar * (-81.00102926445666 + 6.203591096144735 * Ypar))
15341  + Ypar2 * (81.01075991905888 + Ypar * (-58.822719932531164 + 14.670206406369107 * Ypar))
15342  + Wpar2 * (136.70787790194357 + Ypar * (-86.48485007990255 + 35.67671393730628 * Ypar));
15343 
15344  Chi2Tot = Chi2CC13 + Chi2NC27;
15345 
15346  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
15347  return sqrt(Chi2Tot);
15348 }

◆ AuxObs_NP20()

double NPSMEFTd6::AuxObs_NP20 ( ) const
virtual

Auxiliary observable AuxObs_NP20.

Returns
AuxObs_NP20

Reimplemented from NPbase.

Definition at line 16132 of file NPSMEFTd6.cpp.

16133 {
16134  // To be used for some temporary observable
16135  return 0.0;
16136 }

◆ AuxObs_NP3()

double NPSMEFTd6::AuxObs_NP3 ( ) const
virtual

Auxiliary observable AuxObs_NP3 (See code for details.)

Returns
AuxObs_NP3

Reimplemented from NPbase.

Definition at line 15350 of file NPSMEFTd6.cpp.

15351 {
15352  // To be used for some temporary observable
15353 
15354  // WY analysis at 13 TeV for HL-LHC 3/ab for the CC
15355  // WY analysis at 27 TeV for HE-LHC 15/ab for the NC. 1% systematics (corr and uncorr)
15356  double Wpar, Ypar, Wpar2, Ypar2;
15357  double Chi2NC27, Chi2CC13, Chi2Tot;
15358 
15359  Wpar = 10000.0 * obliqueW();
15360  Ypar = 10000.0 * obliqueY();
15361 
15362  Wpar2 = Wpar*Wpar;
15363  Ypar2 = Ypar*Ypar;
15364 
15365  Chi2CC13 = Wpar2 * (18.365037149441695 + 2.422904241798858 * Wpar + 0.12120594308623695 * Wpar2);
15366 
15367  Chi2NC27 = 25.148424251427552 * Wpar2*Wpar2 + Wpar2*Wpar * (-105.31753344410277 + 8.01723084630248 * Ypar)
15368  + Wpar * Ypar * (253.11721255992683 + Ypar * (-93.18990615818014 + 6.8250043104055816 * Ypar))
15369  + Ypar2 * (97.52107126224298 + Ypar * (-67.961770347904945 + 16.80046890875678 * Ypar))
15370  + Wpar2 * (166.84179829911304 + Ypar * (-100.88118582829852 + 41.55424691040131 * Ypar));
15371 
15372  Chi2Tot = Chi2CC13 + Chi2NC27;
15373 
15374  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
15375  return sqrt(Chi2Tot);
15376 }

◆ AuxObs_NP4()

double NPSMEFTd6::AuxObs_NP4 ( ) const
virtual

Auxiliary observable AuxObs_NP4 (See code for details.)

Returns
AuxObs_NP4

Reimplemented from NPbase.

Definition at line 15378 of file NPSMEFTd6.cpp.

15379 {
15380  // WH distribution at 14 TeV: From 1704.01953 + hvqq terms
15381 
15382  double Bin1 = 1.0, Bin2 = 1.0, Bin3 = 1.0, Bin4 = 1.0, Bin5 = 1.0;
15383 
15384  double dVud = 0.0, dVcs = 0.0;
15385  double dcZ = 0.0, cZBox = 0.0, cZZ = 0.0, cZA = 0.0, cAA = 0.0;
15386 
15387  double C11 = 0.0178, C12 = 0.0144, C13 = 0.0102, C14 = 0.0052, C15 = 0.0006;
15388 
15389  double dchi2;
15390 
15391 // Production in each bin (signal strength)
15392 
15393  Bin1 += 12.8 * dVud + 1.75 * dVcs
15394  + 2.00 * dcZ + 5.01 * cZBox + 2.72 * cZZ - 0.0267 * cZA - 0.0217 * cAA;
15395 
15396 // Linear contribution from Higgs self-coupling
15397  Bin1 = Bin1 + cLHd6*(C11 + 2.0*dZH)*deltaG_hhhRatio();
15398 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
15399  Bin1 = Bin1 + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
15400 
15401  Bin2 += 15.3 * dVud + 1.91 * dVcs
15402  + 2.00 * dcZ + 5.81 * cZBox + 3.10 * cZZ - 0.0337 * cZA - 0.0255 * cAA;
15403 
15404 // Linear contribution from Higgs self-coupling
15405  Bin2 = Bin2 + cLHd6*(C12 + 2.0*dZH)*deltaG_hhhRatio();
15406 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
15407  Bin2 = Bin2 + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
15408 
15409  Bin3 += 20.7 * dVud + 2.49 * dVcs
15410  + 2.01 * dcZ + 7.44 * cZBox + 3.76 * cZZ - 0.0535 * cZA - 0.0340 * cAA;
15411 
15412 // Linear contribution from Higgs self-coupling
15413  Bin3 = Bin3 + cLHd6*(C13 + 2.0*dZH)*deltaG_hhhRatio();
15414 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
15415  Bin3 = Bin3 + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
15416 
15417  Bin4 += 35.1 * dVud + 3.63 * dVcs
15418  + 1.98 * dcZ + 11.8 * cZBox + 5.40 * cZZ - 0.112 * cZA - 0.0572 * cAA;
15419 
15420 // Linear contribution from Higgs self-coupling
15421  Bin4 = Bin4 + cLHd6*(C14 + 2.0*dZH)*deltaG_hhhRatio();
15422 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
15423  Bin4 = Bin4 + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
15424 
15425  Bin5 += 67.7 * dVud + 5.41 * dVcs
15426  + 2.03 * dcZ + 22.6 * cZBox + 9.05 * cZZ - 0.276 * cZA - 0.117 * cAA;
15427 
15428 // Linear contribution from Higgs self-coupling
15429  Bin5 = Bin5 + cLHd6*(C15 + 2.0*dZH)*deltaG_hhhRatio();
15430 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
15431  Bin5 = Bin5 + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
15432 
15433 // Compute Chi square using only the last bin and the diphoton, ZZ and bb channels
15434  dchi2 = ( Bin5 * BrHZZ4lRatio() - 1.0 ) * ( Bin5 * BrHZZ4lRatio() - 1.0 )/(0.07*0.07 + 0.48*0.48)
15435  + ( Bin5 * BrHgagaRatio() - 1.0 ) * ( Bin5 * BrHgagaRatio() - 1.0 )/(0.08*0.08 + 0.54*0.54)
15436  + ( Bin5 * BrHbbRatio() - 1.0 ) * ( Bin5 * BrHbbRatio() - 1.0 )/(0.33*0.33 + 0.61*0.61);
15437 
15438  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
15439  return sqrt(dchi2);
15440 }

◆ AuxObs_NP5()

double NPSMEFTd6::AuxObs_NP5 ( ) const
virtual

Auxiliary observable AuxObs_NP5 (See code for details.)

Returns
AuxObs_NP5

Reimplemented from NPbase.

Definition at line 15442 of file NPSMEFTd6.cpp.

15443 {
15444  // ZH distribution at 14 TeV: From 1704.01953 + hvqq terms
15445 
15446  double Bin1 = 1.0, Bin2 = 1.0, Bin3 = 1.0, Bin4 = 1.0, Bin5 = 1.0;
15447 
15448  double dgLZuu = 0.0, dgRZuu = 0.0, dgLZcc = 0.0, dgRZcc = 0.0;
15449  double dgLZdd = 0.0, dgRZdd = 0.0, dgLZss = 0.0, dgRZss = 0.0;
15450 
15451  double dcZ = 0.0, cZBox = 0.0, cZZ = 0.0, cZA = 0.0, cAA = 0.0;
15452 
15453  double C11 = 0.0208, C12 = 0.0164, C13 = 0.0112, C14 = 0.0051, C15 = 0.0021;
15454 
15455  double dchi2;
15456 
15457 // Production in each bin (signal strength)
15458 
15459  Bin1 += 14.6 * dgLZuu - 6.74 * dgRZuu - 11.6 * dgLZdd + 2.28 * dgRZdd
15460  + 1.35 * dgLZcc - 0.589 * dgRZcc - 2.35 * dgLZss + 0.431 * dgRZss
15461  + 2.01 * dcZ + 4.14 * cZBox + 2.12 * cZZ - 0.0237 * cZA - 0.0126 * cAA;
15462 
15463 // Linear contribution from Higgs self-coupling
15464  Bin1 = Bin1 + cLHd6*(C11 + 2.0*dZH)*deltaG_hhhRatio();
15465 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
15466  Bin1 = Bin1 + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
15467 
15468  Bin2 += 16.2 * dgLZuu - 7.77 * dgRZuu - 13.4 * dgLZdd + 2.63 * dgRZdd
15469  + 1.44 * dgLZcc - 0.668 * dgRZcc - 2.52 * dgLZss + 0.462 * dgRZss
15470  + 2.01 * dcZ + 4.86* cZBox + 2.49 * cZZ - 0.0284 * cZA - 0.0156 * cAA;
15471 
15472 // Linear contribution from Higgs self-coupling
15473  Bin2 = Bin2 + cLHd6*(C12 + 2.0*dZH)*deltaG_hhhRatio();
15474 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
15475  Bin2 = Bin2 + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
15476 
15477  Bin3 += 23.0* dgLZuu - 10.8 * dgRZuu - 19.0 * dgLZdd + 3.64 * dgRZdd
15478  + 1.88 * dgLZcc - 0.891 * dgRZcc - 3.19 * dgLZss + 0.591 * dgRZss
15479  + 2.00 * dcZ + 6.35 * cZBox + 3.02 * cZZ - 0.0448 * cZA - 0.0221 * cAA;
15480 
15481 // Linear contribution from Higgs self-coupling
15482  Bin3 = Bin3 + cLHd6*(C13 + 2.0*dZH)*deltaG_hhhRatio();
15483 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
15484  Bin3 = Bin3 + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
15485 
15486  Bin4 += 39.2 * dgLZuu - 18.4 * dgRZuu - 31.4 * dgLZdd + 5.88 * dgRZdd
15487  + 2.78 * dgLZcc - 1.36 * dgRZcc - 4.64 * dgLZss + 0.919 * dgRZss
15488  + 1.98 * dcZ + 10.5 * cZBox + 4.44 * cZZ - 0.0873 * cZA - 0.0396 * cAA;
15489 
15490 // Linear contribution from Higgs self-coupling
15491  Bin4 = Bin4 + cLHd6*(C14 + 2.0*dZH)*deltaG_hhhRatio();
15492 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
15493  Bin4 = Bin4 + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
15494 
15495  Bin5 += 73.4 * dgLZuu - 35.5 * dgRZuu - 58.5 * dgLZdd + 11.2 * dgRZdd
15496  + 4.13 * dgLZcc - 1.95 * dgRZcc - 6.97 * dgLZss + 1.41 * dgRZss
15497  + 1.96 * dcZ + 20.3 * cZBox + 7.27 * cZZ - 0.193 * cZA - 0.0800 * cAA;
15498 
15499 // Linear contribution from Higgs self-coupling
15500  Bin5 = Bin5 + cLHd6*(C15 + 2.0*dZH)*deltaG_hhhRatio();
15501 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
15502  Bin5 = Bin5 + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
15503 
15504 // Compute Chi square using only the last bin and the diphoton, ZZ and bb channels
15505  dchi2 = ( Bin5 * BrHZZ4lRatio() - 1.0 ) * ( Bin5 * BrHZZ4lRatio() - 1.0 )/(0.09*0.09 + 0.65*0.65)
15506  + ( Bin5 * BrHgagaRatio() - 1.0 ) * ( Bin5 * BrHgagaRatio() - 1.0 )/(0.03*0.03 + 0.99*0.99)
15507  + ( Bin5 * BrHbbRatio() - 1.0 ) * ( Bin5 * BrHbbRatio() - 1.0 )/(0.10*0.10 + 0.34*0.34);
15508 
15509  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
15510  return sqrt(dchi2);
15511 }

◆ AuxObs_NP6()

double NPSMEFTd6::AuxObs_NP6 ( ) const
virtual

Auxiliary observable AuxObs_NP6 (See code for details.)

Returns
AuxObs_NP6

Reimplemented from NPbase.

Definition at line 15513 of file NPSMEFTd6.cpp.

15514 {
15515  // To be used for some temporary observable
15516 
15517  // HL-LHC DiHiggs invariant mass distribution: 14 TeV 3/ab
15518 
15519  double Chi2Tot;
15520 
15521 // NP in decays
15522  double dGH2,dGgaga,dGbb, dBRTot;
15523 
15524 // Contributions from the different bins
15525  double Bin1,Bin2,Bin3,Bin4,Bin5,Bin6;
15526  double LLBin1, LLBin2, LLBin3, LLBin4, LLBin5, LLBin6;
15527 
15528 // Higgs basis parameters
15529  double dcZHB,cZboxHB,cZZHB,cZgaHB,cgagaHB,cggHB;
15530  double dytHB,dybHB,dytauHB;
15531  double dKlambda;
15532 
15533  dcZHB = deltacZ_HB();
15534  cZboxHB = cZBox_HB();
15535  cZZHB = cZZ_HB();
15536 
15537 // In the paper it seems they use diff. norm but in the chi 2.nb
15538 // they translate into that convention, so I assume their calculation
15539 // is directly in the HB for the following 3 couplings
15540  cZgaHB = cZga_HB();
15541  cgagaHB = cgaga_HB();
15542  cggHB = cgg_HB();
15543 
15544  dytHB = deltayt_HB();
15545  dybHB = deltayb_HB();
15546  dytauHB = deltaytau_HB();
15547 
15548  dKlambda = deltaG_hhhRatio();
15549 
15550 // Corrections to the different Higgs widths
15551  dGH2 = 1. + 0.010512791990056657 * cZboxHB
15552  - 0.003819752423722165 * cZZHB + 0.0016024991450954641 * cZgaHB
15553  - 0.0005968238492400916 * (2.8975474398595105 * cZboxHB
15554  + 1.8975474398595107 * cZZHB - cZgaHB - 0.3426378481886507 * cgagaHB)
15555  + 0.0990750425382019 * (1.4487737199297552 * cZboxHB + 0.44877371992975534 * cZZHB
15556  - 0.2365019764475461 * cZgaHB - 0.08103452830235015 * cgagaHB)
15557  - 0.0330404571742506 * (cZZHB + 0.4730039528950922 * cZgaHB + 0.055933184863595636 * cgagaHB)
15558  - 0.00033171593951211893 * cgagaHB + 0.48287726036165796 * dcZHB
15559  + 1.1541846695471276 * dybHB + 0.12642022723635785 * dytauHB
15560  + 0.1704272683629381 * (0. + 118.68284969347252 * cggHB
15561  - 0.031082871395970327 * dybHB + 1.034601498835783 * dytHB)
15562  + 0.004560729716754681 * (0. - 12.079950077697095 * cgagaHB
15563  + 1.2739859351743013 * dcZHB + 0.0022136399615102554 * dybHB
15564  - 0.28081416399029446 * dytHB + 0.0036305606562964158 * dytauHB)
15565  + 0.003080492878860618 * (0. - 17.021015025105033 * cZgaHB
15566  + 1.0557935963831278 * dcZHB + 0.0006235357344154619 * dybHB
15567  - 0.05644023795399054 * dytHB + 0.000023105836447458856 * dytauHB);
15568 
15569  dGH2 = dGH2 * dGH2;
15570 
15571  dGgaga = 1.0 + 2.0 * (0. - 12.079950077697095 * cgagaHB
15572  + 1.2739859351743013 * dcZHB + 0.0022136399615102554 * dybHB
15573  - 0.28081416399029446 * dytHB + 0.0036305606562964158 * dytauHB);
15574 
15575  dGbb = 1.0 + 2.0 * dybHB;
15576 
15577  dBRTot = dGbb * dGgaga / dGH2;
15578 
15579  // Bin 1
15580  Bin1 = 0.17*(1.0 + 3.9863794294589585 * cggHB
15581  + 21.333394807321064 * cggHB*cggHB + 3.9527789724382836 * dcZHB
15582  + 0.5566823785534646 * cggHB*dcZHB + 9.077153576669469 * dcZHB*dcZHB
15583  - 7.713285621354339 * dytHB + 6.573887966178747 * cggHB*dytHB
15584  - 45.88983201032187 * dcZHB*dytHB + 62.42156375416841 * dytHB*dytHB
15585  + 4.257555672380181 * cggHB*dytHB*dytHB + 4.620310477256665 * dcZHB*dytHB*dytHB
15586  - 9.403185493195476 * dytHB*dytHB*dytHB + 1.1563473213070041 * dytHB*dytHB*dytHB*dytHB
15587  - 0.14505129596051047 * dKlambda - 0.1418831193390564 * cggHB*dKlambda
15588  + 1.3502693869386464 * cggHB*cggHB*dKlambda - 0.6675315048183816 * dcZHB*dKlambda
15589  - 0.002999558395846163 * cggHB*dcZHB*dKlambda
15590  + 1.5448485758806263 * dytHB * dKlambda
15591  - 0.005002986050963205 * cggHB*dytHB*dKlambda
15592  - 0.6675315048183816 * dcZHB*dytHB * dKlambda
15593  + 1.5222565251876392 * dytHB*dytHB * dKlambda
15594  + 0.1278814581005547 * cggHB*dytHB*dytHB * dKlambda
15595  - 0.1676433466534976 * dytHB*dytHB*dytHB * dKlambda
15596  + 0.011296025346493552 * dKlambda*dKlambda
15597  + 0.0014116654816114353 * cggHB*dKlambda*dKlambda
15598  + 0.022260157195710357 * cggHB*cggHB*dKlambda*dKlambda
15599  + 0.022592050692987104 * dytHB * dKlambda*dKlambda
15600  + 0.0014116654816114353 * cggHB*dytHB*dKlambda*dKlambda
15601  + 0.011296025346493552 * dytHB*dytHB * dKlambda*dKlambda);
15602 
15603  Bin1 = 0.67944 + Bin1 * dBRTot;
15604 
15605  // Exclude points with negative values of BinX
15606  if ( Bin1 < 0 ) return std::numeric_limits<double>::quiet_NaN();
15607 
15608  // Delta chi2 = -2*LL for the bin
15609  // Add an abs in the denominator of the log,
15610  // even if events with negative BinX are not supposed to reach here.
15611  LLBin1 = 2.0 * (Bin1 - 0.84944 + 0.84944 * log( 0.84944 / fabs(Bin1) ) );
15612 
15613  // Bin 2
15614  Bin2 = 0.33*(1.0 + 1.8019627645351037 * cggHB
15615  + 7.953163597932105 * cggHB*cggHB + 3.735123481549394 * dcZHB
15616  - 2.654186900737259 * cggHB*dcZHB + 6.403420811368324 * dcZHB*dcZHB
15617  - 6.991501690350679 * dytHB + 11.425848100026737 * cggHB*dytHB
15618  - 30.219763494155394 * dcZHB*dytHB + 39.692409895713936 * dytHB*dytHB
15619  + 1.661324633279857 * cggHB*dytHB*dytHB + 4.46563789250516 * dcZHB*dytHB*dytHB
15620  - 8.710706509282613 * dytHB*dytHB*dytHB + 1.2361692069676826 * dytHB*dytHB*dytHB*dytHB
15621  - 0.21386875429750188 * dKlambda + 0.2363972133088796 * cggHB*dKlambda
15622  + 0.8549707073528667 * cggHB*cggHB*dKlambda - 0.7305144109557659 * dcZHB*dKlambda
15623  - 0.14136602060890807 * cggHB*dcZHB*dKlambda + 1.50533606463443 * dytHB * dKlambda
15624  + 0.747017712869579 * cggHB*dytHB*dKlambda - 0.7305144109557659 * dcZHB*dytHB * dKlambda
15625  + 1.4607351592940678 * dytHB*dytHB * dKlambda
15626  + 0.08652243773397514 * cggHB*dytHB*dytHB * dKlambda
15627  - 0.25846965963786395 * dytHB*dytHB*dytHB * dKlambda
15628  + 0.022300452670181038 * dKlambda*dKlambda + 0.009236644319657653 * cggHB*dKlambda*dKlambda
15629  + 0.023125582948149842 * cggHB*cggHB*dKlambda*dKlambda
15630  + 0.044600905340362075 * dytHB * dKlambda*dKlambda
15631  + 0.009236644319657653 * cggHB*dytHB*dKlambda*dKlambda
15632  + 0.022300452670181038 * dytHB*dytHB * dKlambda*dKlambda) ;
15633 
15634  Bin2 = 1.4312 + Bin2 * dBRTot;
15635 
15636  // Exclude points with negative values of BinX
15637  if ( Bin2 < 0 ) return std::numeric_limits<double>::quiet_NaN();
15638 
15639  // Delta chi2 = -2*LL for the bin
15640  // Add an abs in the denominator of the log,
15641  // even if events with negative BinX are not supposed to reach here.
15642  LLBin2 = 2.0 * (Bin2 - 1.7612 + 1.7612 * log( 1.7612 / fabs(Bin2) ) );
15643 
15644  // Bin 3
15645  Bin3 = 0.99*(1.0 + 0.6707152151845268 * cggHB
15646  + 4.113022405261353 * cggHB*cggHB + 3.4241906309399726 * dcZHB
15647  - 2.9926046286644703 * cggHB*dcZHB + 4.72026565086762 * dcZHB*dcZHB
15648  - 5.98522416048399 * dytHB + 10.012680455917307 * cggHB*dytHB
15649  - 20.69102310585157 * dcZHB*dytHB + 26.4871108999121 * dytHB*dytHB
15650  + 0.36415135473936855 * cggHB*dytHB*dytHB
15651  + 4.206380168414172 * dcZHB*dytHB*dytHB - 7.688318821918381 * dytHB*dytHB*dytHB
15652  + 1.3217369754941033 * dytHB*dytHB*dytHB*dytHB - 0.2873477323359291 * dKlambda
15653  + 0.35631144357921507 * cggHB*dKlambda
15654  + 0.6197019283831009 * cggHB*cggHB*dKlambda
15655  - 0.7821895374741993 * dcZHB*dKlambda
15656  - 0.23172596419155064 * cggHB*dcZHB*dKlambda
15657  + 1.415746929098462 * dytHB * dKlambda
15658  + 1.0816714186441074 * cggHB*dytHB*dKlambda
15659  - 0.7821895374741993 * dcZHB*dytHB * dKlambda
15660  + 1.3469684427821131 * dytHB*dytHB * dKlambda
15661  + 0.030182082490240562 * cggHB*dytHB*dytHB * dKlambda
15662  - 0.35612621865227795 * dytHB*dytHB*dytHB * dKlambda
15663  + 0.03438924315817444 * dKlambda*dKlambda
15664  + 0.019565500643816278 * cggHB*dKlambda*dKlambda
15665  + 0.02382411268034237 * cggHB*cggHB*dKlambda*dKlambda
15666  + 0.06877848631634888 * dytHB * dKlambda*dKlambda
15667  + 0.019565500643816278 * cggHB*dytHB*dKlambda*dKlambda
15668  + 0.03438924315817444 * dytHB*dytHB * dKlambda*dKlambda);
15669 
15670  Bin3 = 1.9764 + Bin3 * dBRTot;
15671 
15672  // Exclude points with negative values of BinX
15673  if ( Bin3 < 0 ) return std::numeric_limits<double>::quiet_NaN();
15674 
15675  // Delta chi2 = -2*LL for the bin
15676  // Add an abs in the denominator of the log,
15677  // even if events with negative BinX are not supposed to reach here.
15678  LLBin3 = 2.0 * (Bin3 - 2.9664 + 2.9664 * log( 2.9664 / fabs(Bin3) ) );
15679 
15680  // Bin 4
15681  Bin4 = 2.86*(1.0 - 0.27406342847042814 * cggHB
15682  + 1.9597360046161074 * cggHB*cggHB + 3.0113078755334115 * dcZHB
15683  - 2.776019265892887 * cggHB*dcZHB + 3.1917709639679823 * dcZHB*dcZHB
15684  - 4.6362529563760955 * dytHB + 7.377234185667426 * cggHB*dytHB
15685  - 12.294598143269557 * dcZHB*dytHB + 15.407456380301479 * dytHB*dytHB
15686  - 0.6767601835408067 * cggHB*dytHB*dytHB
15687  + 3.844719765004924 * dcZHB*dytHB*dytHB
15688  - 6.227970053277897 * dytHB*dytHB*dytHB + 1.4542592857563688 * dytHB*dytHB*dytHB*dytHB
15689  - 0.39767067022413716 * dKlambda + 0.3661464075997459 * cggHB*dKlambda
15690  + 0.4464409042746693 * cggHB*cggHB*dKlambda
15691  - 0.8334118894715125 * dcZHB*dKlambda
15692  - 0.3263197431214281 * cggHB*dcZHB*dKlambda
15693  + 1.1940464266776625 * dytHB * dKlambda
15694  + 1.2643073873631234 * cggHB*dytHB*dKlambda
15695  - 0.8334118894715125 * dcZHB*dytHB * dKlambda
15696  + 1.0808691956131988 * dytHB*dytHB * dKlambda
15697  - 0.0807982496009068 * cggHB*dytHB*dytHB * dKlambda
15698  - 0.5108479012886007 * dytHB*dytHB*dytHB * dKlambda
15699  + 0.05658861553223176 * dKlambda*dKlambda
15700  + 0.04424790213027415 * cggHB*dKlambda*dKlambda
15701  + 0.02585578262020257 * cggHB*cggHB*dKlambda*dKlambda
15702  + 0.11317723106446352 * dytHB * dKlambda*dKlambda
15703  + 0.04424790213027415 * cggHB*dytHB*dKlambda*dKlambda
15704  + 0.05658861553223176 * dytHB*dytHB * dKlambda*dKlambda);
15705 
15706  Bin4 = 5.167 + Bin4 * dBRTot;
15707 
15708  // Exclude points with negative values of BinX
15709  if ( Bin4 < 0 ) return std::numeric_limits<double>::quiet_NaN();
15710 
15711  // Delta chi2 = -2*LL for the bin
15712  // Add an abs in the denominator of the log,
15713  // even if events with negative BinX are not supposed to reach here.
15714  LLBin4 = 2.0 * (Bin4 - 8.027 + 8.027 * log( 8.027 / fabs(Bin4) ) );
15715 
15716  // Bin 5
15717  Bin5 = 6.34* (1.0 - 1.094329254675176 * cggHB
15718  + 1.0393648302909912 * cggHB*cggHB + 2.6000916816530903 * dcZHB
15719  - 2.4448264513323226 * cggHB*dcZHB + 2.073935963891534 * dcZHB*dcZHB
15720  - 3.192332240205929 * dytHB + 4.5914586198385 * cggHB*dytHB
15721  - 6.2871857258718595 * dcZHB*dytHB + 8.134770266934664 * dytHB*dytHB
15722  - 1.648691479483292 * cggHB*dytHB*dytHB + 3.5563383758242524 * dcZHB*dytHB*dytHB
15723  - 4.615570013047001 * dytHB*dytHB*dytHB + 1.7227511548362076 * dytHB*dytHB*dytHB*dytHB
15724  - 0.6079428047533413 * dKlambda + 0.33825211279194234 * cggHB*dKlambda
15725  + 0.3879052211526028 * cggHB*cggHB*dKlambda - 0.956246694171162 * dcZHB*dKlambda
15726  - 0.4572431444456198 * cggHB*dcZHB*dKlambda + 0.8152949680877302 * dytHB * dKlambda
15727  + 1.3814632626914451 * cggHB*dytHB*dKlambda
15728  - 0.956246694171162 * dcZHB*dytHB * dKlambda + 0.5856782679219981 * dytHB*dytHB * dKlambda
15729  - 0.3285182834373566 * cggHB*dytHB*dytHB * dKlambda
15730  - 0.8375595049190734 * dytHB*dytHB*dytHB * dKlambda + 0.11480835008286604 * dKlambda*dKlambda
15731  + 0.11240817142118299 * cggHB*dKlambda*dKlambda + 0.03688252014841459 * cggHB*cggHB*dKlambda*dKlambda
15732  + 0.22961670016573207 * dytHB * dKlambda*dKlambda
15733  + 0.11240817142118299 * cggHB*dytHB*dKlambda*dKlambda
15734  + 0.11480835008286604 * dytHB*dytHB * dKlambda*dKlambda);
15735 
15736  Bin5 = 15.93 + Bin5 * dBRTot;
15737 
15738  // Exclude points with negative values of BinX
15739  if ( Bin5 < 0 ) return std::numeric_limits<double>::quiet_NaN();
15740 
15741  // Delta chi2 = -2*LL for the bin
15742  // Add an abs in the denominator of the log,
15743  // even if events with negative BinX are not supposed to reach here.
15744  LLBin5 = 2.0 * (Bin5 - 22.27 + 22.27 * log( 22.27 / fabs(Bin5) ) );
15745 
15746  // Bin 6
15747  Bin6 = 2.14*(1.0 - 2.007855065799201 * cggHB + 1.1994575008850934 * cggHB*cggHB
15748  + 2.5987763498382352 * dcZHB - 2.908713303420072 * cggHB*dcZHB
15749  + 1.804645897901265 * dcZHB*dcZHB - 2.806900956988577 * dytHB
15750  + 3.5621616844486415 * cggHB*dytHB - 4.250685020965587 * dcZHB*dytHB
15751  + 5.7468374752045515 * dytHB*dytHB - 3.1561231600123736 * cggHB*dytHB*dytHB
15752  + 3.9784140166037667 * dcZHB*dytHB*dytHB - 4.4303353405513395 * dytHB*dytHB*dytHB
15753  + 2.257739308366916 * dytHB*dytHB*dytHB*dytHB - 0.9894280925261291 * dKlambda
15754  + 0.589956279744333 * cggHB*dKlambda + 0.6687315933211253 * cggHB*cggHB*dKlambda
15755  - 1.3796376667655315 * dcZHB*dKlambda - 0.8069993678124955 * cggHB*dcZHB*dKlambda
15756  + 0.6340062910366335 * dytHB * dKlambda + 2.127573647123277 * cggHB*dytHB*dKlambda
15757  - 1.3796376667655315 * dcZHB*dytHB * dKlambda + 0.09738385935505989 * dytHB*dytHB * dKlambda
15758  - 0.8833807360585424 * cggHB*dytHB*dytHB * dKlambda - 1.5260505242077027 * dytHB*dytHB*dytHB * dKlambda
15759  + 0.2683112158407868 * dKlambda*dKlambda + 0.32506892158970235 * cggHB*dKlambda*dKlambda
15760  + 0.09418943796384227 * cggHB*cggHB*dKlambda*dKlambda + 0.5366224316815736 * dytHB * dKlambda*dKlambda
15761  + 0.32506892158970235 * cggHB*dytHB*dKlambda*dKlambda
15762  + 0.2683112158407868 * dytHB*dytHB * dKlambda*dKlambda);
15763 
15764  Bin6 = 12.01 + Bin6 * dBRTot;
15765 
15766  // Exclude points with negative values of BinX
15767  if ( Bin6 < 0 ) return std::numeric_limits<double>::quiet_NaN();
15768 
15769  // Delta chi2 = -2*LL for the bin
15770  // Add an abs in the denominator of the log,
15771  // even if events with negative BinX are not supposed to reach here.
15772  LLBin6 = 2.0 * (Bin6 - 14.15 + 14.15 * log( 14.15 / fabs(Bin6) ) );
15773 
15774  // The total contributions to the log-likelihood/chi-square
15775  Chi2Tot = LLBin1 + LLBin2 + LLBin3 + LLBin4 + LLBin5 + LLBin6;
15776 
15777  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
15778  return sqrt(Chi2Tot);
15779 }

◆ AuxObs_NP7()

double NPSMEFTd6::AuxObs_NP7 ( ) const
virtual

Auxiliary observable AuxObs_NP7 (See code for details.)

Returns
AuxObs_NP7

Reimplemented from NPbase.

Definition at line 15781 of file NPSMEFTd6.cpp.

15782 {
15783  // To be used for some temporary observable
15784 
15785  // CLIC STWY using difermion production at all energies: 380, 1500 and 3000 GeV
15786  double Spar, Tpar, Wpar, Ypar, Spar2, Tpar2, Wpar2, Ypar2;
15787  double Chi2Tot;
15788 
15789  Spar = obliqueS();
15790  Tpar = obliqueT();
15791  Wpar = 10000.0 * obliqueW();
15792  Ypar = 10000.0 * obliqueY();
15793 
15794  Spar2 = Spar*Spar;
15795  Tpar2 = Tpar*Tpar;
15796  Wpar2 = Wpar*Wpar;
15797  Ypar2 = Ypar*Ypar;
15798 
15799  Chi2Tot = 442.84977653097394 * Spar2
15800  - 728.5215604181935 * Spar * Tpar
15801  + 404.15957807101813 * Tpar2
15802  + 400.03987723904224 * Spar * Wpar
15803  - 639.6154242400826 * Tpar * Wpar
15804  + 4337.791457515823 * Wpar2
15805  - 106.87313892453362 * Spar * Ypar
15806  - 72.94355609762007 * Tpar * Ypar
15807  + 3002.848116515672 * Wpar * Ypar
15808  + 3040.1630882458923 * Ypar2;
15809 
15810  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
15811  return sqrt(Chi2Tot);
15812 }

◆ AuxObs_NP8()

double NPSMEFTd6::AuxObs_NP8 ( ) const
virtual

Auxiliary observable AuxObs_NP8 (See code for details.)

Returns
AuxObs_NP8

Reimplemented from NPbase.

Definition at line 15814 of file NPSMEFTd6.cpp.

15815 {
15816  // To be used for some temporary observable
15817 
15818  // CLIC DiHiggs: exclusive analysis. Full CLIC run
15819  double Chi2Tot;
15820 
15821 // Higgs basis parameters
15822  double dKlambda;
15823 
15824  dKlambda = deltaG_hhhRatio();
15825 
15826  Chi2Tot = dKlambda * dKlambda * (50.04473972806045
15827  - 104.47283225861888 * dKlambda
15828  + 84.48333683635175 * dKlambda*dKlambda );
15829 
15830  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
15831  return sqrt(Chi2Tot);
15832 }

◆ AuxObs_NP9()

double NPSMEFTd6::AuxObs_NP9 ( ) const
virtual

Auxiliary observable AuxObs_NP9 (See code for details.)

Returns
AuxObs_NP9

Reimplemented from NPbase.

Definition at line 15834 of file NPSMEFTd6.cpp.

15835 {
15836  // To be used for some temporary observable
15837 
15838  // ILC DiHiggs at 500 GeV: 2/ab per polarization (+-80,-+30)
15839 
15840  double Chi2p80m30, Chi2m80p30, Chi2Tot;
15841 
15842 // Higgs basis parameters
15843  double dcZHB,cZboxHB,cZZHB,cZgaHB,cgagaHB;
15844  double dKlambda;
15845 
15846  dcZHB = deltacZ_HB();
15847  cZboxHB = cZBox_HB();
15848  cZZHB = cZZ_HB();
15849  cZgaHB = cZga_HB();
15850  cgagaHB = cgaga_HB();
15851 
15852  dKlambda = deltaG_hhhRatio();
15853 
15854 // The signal strength -1
15855  Chi2p80m30 = 13.6982 * cZZHB
15856  - 7.58943 * cZgaHB
15857  + 14.6843 * cZboxHB
15858  - 1.51882 * cgagaHB
15859  + 5.46836 * dcZHB
15860  + 0.565585 * dKlambda
15861  + 0.000631004 * cZZHB * dKlambda
15862  - 0.195079 * cZgaHB * dKlambda
15863  + 0.064441 * cZboxHB * dKlambda
15864  + 0.440061 * cgagaHB * dKlambda
15865  + 2.13192 * dcZHB * dKlambda
15866  + 0.0968208 * dKlambda * dKlambda;
15867 
15868 // ILC report (1903.01629) gives total cross section a 4/ab: 16.8%.
15869 // Assume the precision for each polarization is the same as they do for single Higgs in ZH...
15870  Chi2p80m30 = Chi2p80m30 * Chi2p80m30 / 0.168 / 0.168 / 2.0;
15871 
15872 // The signal strength -1
15873  Chi2m80p30 = - 2.57112 * cZZHB
15874  + 6.97966 * cZgaHB
15875  - 10.2626 * cZboxHB
15876  + 1.39647 * cgagaHB
15877  + 5.4684 * dcZHB
15878  + 0.565577 * dKlambda
15879  + 4.71916 * cZZHB * dKlambda
15880  + 0.179045 * cZgaHB * dKlambda
15881  + 7.28766 * cZboxHB * dKlambda
15882  - 0.405166 * cgagaHB * dKlambda
15883  + 2.13189 * dcZHB * dKlambda
15884  + 0.0968201 * dKlambda * dKlambda;
15885 
15886 // ILC report (1903.01629) gives total cross section a 4/ab: 16.8%.
15887 // Assume the precision for each polarization is the same as they do for single Higgs in ZH...
15888  Chi2m80p30 = Chi2m80p30 * Chi2m80p30 / 0.168 / 0.168 / 2.0;
15889 
15890  Chi2Tot = Chi2p80m30 + Chi2m80p30;
15891 
15892  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
15893  return sqrt(Chi2Tot);
15894 }

◆ bPskPol()

double NPSMEFTd6::bPskPol ( const double  sqrt_s,
const double  Pol_em,
const double  Pol_ep 
) const
virtual

the angular parameter \(b\) from \(\mu_{e^+e^- \to ZH}\) (arXiv:1708.09079 [hep-ph]).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively
Returns
\(b_{eeZH}\)

Reimplemented from NPbase.

Definition at line 8698 of file NPSMEFTd6.cpp.

8699 {
8700  double bL, bR, bPol;
8701  double sM = sqrt_s * sqrt_s;
8702  double Mz2 = Mz*Mz;
8703 
8704  double ZetaZ, ZetaAZ;
8705  double CWB, CBB, CWW;
8706 
8707  // Convention for dim 6 operators
8709  CBB = 0.25 * (g2_tree*g2_tree/g1_tree/g1_tree) * CiHB * v2_over_LambdaNP2;
8710  CWW = 0.25 * CiHW * v2_over_LambdaNP2;
8711 
8712  ZetaZ = cW2_tree*8.0*CWW + 2.0*sW2_tree*8*CWB + (sW2_tree*sW2_tree/cW2_tree)*8.0*CBB;
8713  ZetaAZ = sW_tree*cW_tree*(8.0*CWW - (1.0 - sW2_tree/cW2_tree)*8*CWB - (sW2_tree/cW2_tree)*8.0*CBB);
8714 
8715  // LH and RH pars
8716  bL = ZetaZ + (sW_tree*cW_tree)/(0.5 - sW2_tree)*(sM - Mz2)/sM*ZetaAZ;
8717  bR = ZetaZ - (cW_tree/sW_tree)*(sM - Mz2)/sM*ZetaAZ;
8718 
8719  // Polarized b parameter
8720  bPol = 0.25 * ( (1.0 - Pol_em/100.0)*(1.0 + Pol_ep/100.0) * bL
8721  + (1.0 + Pol_em/100.0)*(1.0 - Pol_ep/100.0) * bR );
8722 
8723  return bPol;
8724 }

◆ Br_H_exo()

double NPSMEFTd6::Br_H_exo ( ) const
virtual

The branching ratio of the of the Higgs into exotic particles.

Returns
Br \((H\to exotic)\)

Reimplemented from NPbase.

Definition at line 12389 of file NPSMEFTd6.cpp.

12390 {
12391  if (BrHexo < 0) return std::numeric_limits<double>::quiet_NaN();
12392 
12393  return BrHexo;
12394 }

◆ Br_H_inv()

double NPSMEFTd6::Br_H_inv ( ) const
virtual

The branching ratio of the of the Higgs into invisible particles.

Returns
Br \((H\to invisible)\)

Reimplemented from NPbase.

Definition at line 12396 of file NPSMEFTd6.cpp.

12397 {
12398 // Contributions from both modifications in H->ZZ->4v and the extra invisible decays
12399  double BR4v;
12400 
12401  BR4v = BrHZZ4vRatio()*(trueSM.computeBrHtoZZinv());
12402 
12403 // BR4v positivity is already checked inside BrHZZ4vRatio()
12404 // and will be nan if negative. Check here BrHinv, to make sure both are positive
12405  if (BrHinv < 0) return std::numeric_limits<double>::quiet_NaN();
12406 
12407  return BR4v + BrHinv;
12408 }

◆ Br_H_inv_NP()

double NPSMEFTd6::Br_H_inv_NP ( ) const
virtual

The branching ratio of the of the Higgs into invisible particles (only invisible new particles).

Returns
Br \((H\to invisible,NP)\)

Reimplemented from NPbase.

Definition at line 12411 of file NPSMEFTd6.cpp.

12412 {
12413 
12414 // BR4v positivity is already checked inside BrHZZ4vRatio()
12415 // and will be nan if negative. Check here BrHinv, to make sure both are positive
12416  if (BrHinv < 0) return std::numeric_limits<double>::quiet_NaN();
12417 
12418  return BrHinv;
12419 }

◆ BrHbbRatio()

double NPSMEFTd6::BrHbbRatio ( ) const
virtual

The ratio of the Br \((H\to b\bar{b})\) in the current model and in the Standard Model.

Returns
Br \((H\to b\bar{b})\)/Br \((H\to b\bar{b})_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10542 of file NPSMEFTd6.cpp.

10543 {
10544  double Br = 1.0;
10545  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10546 
10547  dGHiR1= deltaGammaHbbRatio1();
10548 
10549  Br += dGHiR1 - dGammaHTotR1;
10550 
10551  if (FlagQuadraticTerms) {
10552 
10553  dGHiR2= deltaGammaHbbRatio2();
10554 
10555  //Add contributions that are quadratic in the effective coefficients
10556  Br += - dGHiR1 * dGammaHTotR1
10557  + dGHiR2 - dGammaHTotR2
10558  + pow(dGammaHTotR1,2.0);
10559  }
10560 
10561  GHiR += dGHiR1 + dGHiR2;
10562  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10563 
10564  return Br;
10565 
10566 }

◆ BrHccRatio()

double NPSMEFTd6::BrHccRatio ( ) const
virtual

The ratio of the Br \((H\to c\bar{c})\) in the current model and in the Standard Model.

Returns
Br \((H\to c\bar{c})\)/Br \((H\to c\bar{c})_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10516 of file NPSMEFTd6.cpp.

10517 {
10518  double Br = 1.0;
10519  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10520 
10521  dGHiR1= deltaGammaHccRatio1();
10522 
10523  Br += dGHiR1 - dGammaHTotR1;
10524 
10525  if (FlagQuadraticTerms) {
10526 
10527  dGHiR2= deltaGammaHccRatio2();
10528 
10529  //Add contributions that are quadratic in the effective coefficients
10530  Br += - dGHiR1 * dGammaHTotR1
10531  + dGHiR2 - dGammaHTotR2
10532  + pow(dGammaHTotR1,2.0);
10533  }
10534 
10535  GHiR += dGHiR1 + dGHiR2;
10536  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10537 
10538  return Br;
10539 
10540 }

◆ BrHgagaRatio()

double NPSMEFTd6::BrHgagaRatio ( ) const
virtual

The ratio of the Br \((H\to \gamma\gamma)\) in the current model and in the Standard Model.

Returns
Br \((H\to \gamma\gamma)\)/Br \((H\to \gamma\gamma)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10438 of file NPSMEFTd6.cpp.

10439 {
10440  double Br = 1.0;
10441  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10442 
10443  dGHiR1= deltaGammaHgagaRatio1();
10444 
10445  Br += dGHiR1 - dGammaHTotR1;
10446 
10447  if (FlagQuadraticTerms) {
10448 
10449  dGHiR2= deltaGammaHgagaRatio2();
10450 
10451  //Add contributions that are quadratic in the effective coefficients
10452  Br += - dGHiR1 * dGammaHTotR1
10453  + dGHiR2 - dGammaHTotR2
10454  + pow(dGammaHTotR1,2.0);
10455  }
10456 
10457  GHiR += dGHiR1 + dGHiR2;
10458  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10459 
10460  return Br;
10461 
10462 }

◆ BrHggRatio()

double NPSMEFTd6::BrHggRatio ( ) const
virtual

The ratio of the Br \((H\to gg)\) in the current model and in the Standard Model.

Returns
Br \((H\to gg)\)/Br \((H\to gg)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 9878 of file NPSMEFTd6.cpp.

9879 {
9880  double Br = 1.0;
9881  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
9882 
9883  dGHiR1= deltaGammaHggRatio1();
9884 
9885  Br += dGHiR1 - dGammaHTotR1;
9886 
9887  if (FlagQuadraticTerms) {
9888 
9889  dGHiR2= deltaGammaHggRatio2();
9890 
9891  //Add contributions that are quadratic in the effective coefficients
9892  Br += - dGHiR1 * dGammaHTotR1
9893  + dGHiR2 - dGammaHTotR2
9894  + pow(dGammaHTotR1,2.0);
9895  }
9896 
9897  GHiR += dGHiR1 + dGHiR2;
9898  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
9899 
9900  return Br;
9901 
9902 }

◆ BrHmumuRatio()

double NPSMEFTd6::BrHmumuRatio ( ) const
virtual

The ratio of the Br \((H\to \mu^+\mu^-)\) in the current model and in the Standard Model.

Returns
Br \((H\to \mu^+\mu^-)\)/Br \((H\to \mu^+\mu^-)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10464 of file NPSMEFTd6.cpp.

10465 {
10466  double Br = 1.0;
10467  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10468 
10469  dGHiR1= deltaGammaHmumuRatio1();
10470 
10471  Br += dGHiR1 - dGammaHTotR1;
10472 
10473  if (FlagQuadraticTerms) {
10474 
10475  dGHiR2= deltaGammaHmumuRatio2();
10476 
10477  //Add contributions that are quadratic in the effective coefficients
10478  Br += - dGHiR1 * dGammaHTotR1
10479  + dGHiR2 - dGammaHTotR2
10480  + pow(dGammaHTotR1,2.0);
10481  }
10482 
10483  GHiR += dGHiR1 + dGHiR2;
10484  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10485 
10486  return Br;
10487 
10488 }

◆ BrHtautauRatio()

double NPSMEFTd6::BrHtautauRatio ( ) const
virtual

The ratio of the Br \((H\to \tau^+\tau^-)\) in the current model and in the Standard Model.

Returns
Br \((H\to \tau^+\tau^-)\)/Br \((H\to \tau^+\tau^-)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10490 of file NPSMEFTd6.cpp.

10491 {
10492  double Br = 1.0;
10493  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10494 
10495  dGHiR1= deltaGammaHtautauRatio1();
10496 
10497  Br += dGHiR1 - dGammaHTotR1;
10498 
10499  if (FlagQuadraticTerms) {
10500 
10501  dGHiR2= deltaGammaHtautauRatio2();
10502 
10503  //Add contributions that are quadratic in the effective coefficients
10504  Br += - dGHiR1 * dGammaHTotR1
10505  + dGHiR2 - dGammaHTotR2
10506  + pow(dGammaHTotR1,2.0);
10507  }
10508 
10509  GHiR += dGHiR1 + dGHiR2;
10510  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10511 
10512  return Br;
10513 
10514 }

◆ BrHtoinvRatio()

double NPSMEFTd6::BrHtoinvRatio ( ) const
virtual

The ratio of the Br \((H\to invisible)\) in the current model and in the Standard Model.

Returns
Br \((H\to invisible)\)/Br \((H\to ZZ \to invisible)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 12470 of file NPSMEFTd6.cpp.

12471 {
12472  return (Br_H_inv()/(trueSM.computeBrHtoZZinv()));
12473 }

◆ BrHvisRatio()

double NPSMEFTd6::BrHvisRatio ( ) const
virtual

The ratio of the Br \((H\to visible)\) in the current model and in the Standard Model.

Returns
Br \((H\to visible)\)/Br \((H\to visible)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 12422 of file NPSMEFTd6.cpp.

12423 {
12424  double Br = 1.0;
12425  double dvis1 = 0.0, dvis2 = 0.0, delta2SM;
12426  double GHvisR = 1.0;
12427 
12428 // Sum over decays of visible SM and exotic modes
12438  + BrHexo);
12439 
12440  Br += dvis1 - dGammaHTotR1;
12441 
12442  if (FlagQuadraticTerms) {
12443 
12444 // Sum over decays of visible SM and exotic modes
12445  delta2SM = trueSM.computeBrHtogg() * deltaGammaHggRatio2()
12454 
12455  dvis2 = delta2SM + (BrHexo)*(BrHexo + delta2SM);
12456 
12457  //Add contributions that are quadratic in the effective coefficients
12458  Br += - dvis1 * dGammaHTotR1
12459  + dvis2 - dGammaHTotR2
12460  + pow(dGammaHTotR1,2.0);
12461  }
12462 
12463  GHvisR += dvis1 + dvis2;
12464  if ((Br < 0) || (GHvisR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
12465 
12466  return Br;
12467 }

◆ BrHWffRatio()

double NPSMEFTd6::BrHWffRatio ( ) const
virtual

The ratio of the Br \((H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model.

Returns
Br \((H\to W f f)\)/Br \((H\to W f f)_{\mathrm{SM}}\)

Definition at line 10011 of file NPSMEFTd6.cpp.

10012 {
10013  double Br = 1.0;
10014  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10015 
10016  dGHiR1= deltaGammaHWffRatio1();
10017 
10018  Br += dGHiR1 - dGammaHTotR1;
10019 
10020  if (FlagQuadraticTerms) {
10021 
10022  dGHiR2= deltaGammaHWffRatio2();
10023 
10024  //Add contributions that are quadratic in the effective coefficients
10025  Br += - dGHiR1 * dGammaHTotR1
10026  + dGHiR2 - dGammaHTotR2
10027  + pow(dGammaHTotR1,2.0);
10028  }
10029 
10030  GHiR += dGHiR1 + dGHiR2;
10031  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10032 
10033  return Br;
10034 }

◆ BrHWjjRatio()

double NPSMEFTd6::BrHWjjRatio ( ) const
virtual

The ratio of the Br \((H\to W j j)\) in the current model and in the Standard Model.

Returns
Br \((H\to W j j)\)/Br \((H\to W j j)_{\mathrm{SM}}\)

Definition at line 9961 of file NPSMEFTd6.cpp.

9962 {
9963  double Br = 1.0;
9964  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
9965 
9966  dGHiR1= deltaGammaHWjjRatio1();
9967 
9968  Br += dGHiR1 - dGammaHTotR1;
9969 
9970  if (FlagQuadraticTerms) {
9971 
9972  dGHiR2= deltaGammaHWjjRatio2();
9973 
9974  //Add contributions that are quadratic in the effective coefficients
9975  Br += - dGHiR1 * dGammaHTotR1
9976  + dGHiR2 - dGammaHTotR2
9977  + pow(dGammaHTotR1,2.0);
9978  }
9979 
9980  GHiR += dGHiR1 + dGHiR2;
9981  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
9982 
9983  return Br;
9984 }

◆ BrHWlvRatio()

double NPSMEFTd6::BrHWlvRatio ( ) const
virtual

The ratio of the Br \((H\to W l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.

Returns
Br \((H\to Wl\nu)\)/Br \((H\to Wl\nu)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 9911 of file NPSMEFTd6.cpp.

9912 {
9913  double Br = 1.0;
9914  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
9915 
9916  dGHiR1= deltaGammaHWlvRatio1();
9917 
9918  Br += dGHiR1 - dGammaHTotR1;
9919 
9920  if (FlagQuadraticTerms) {
9921 
9922  dGHiR2= deltaGammaHWlvRatio2();
9923 
9924  //Add contributions that are quadratic in the effective coefficients
9925  Br += - dGHiR1 * dGammaHTotR1
9926  + dGHiR2 - dGammaHTotR2
9927  + pow(dGammaHTotR1,2.0);
9928  }
9929 
9930  GHiR += dGHiR1 + dGHiR2;
9931  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
9932 
9933  return Br;
9934 }

◆ BrHWW2l2vRatio()

double NPSMEFTd6::BrHWW2l2vRatio ( ) const
virtual

The ratio of the Br \((H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.

Returns
Br \((H\to WW^*\to l\nu l\nu)\)/Br \((H\to WW^*\to l\nu l\nu)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 9936 of file NPSMEFTd6.cpp.

9937 {
9938  double Br = 1.0;
9939  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
9940 
9941  dGHiR1= deltaGammaHWW2l2vRatio1();
9942 
9943  Br += dGHiR1 - dGammaHTotR1;
9944 
9945  if (FlagQuadraticTerms) {
9946 
9947  dGHiR2= deltaGammaHWW2l2vRatio2();
9948 
9949  //Add contributions that are quadratic in the effective coefficients
9950  Br += - dGHiR1 * dGammaHTotR1
9951  + dGHiR2 - dGammaHTotR2
9952  + pow(dGammaHTotR1,2.0);
9953  }
9954 
9955  GHiR += dGHiR1 + dGHiR2;
9956  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
9957 
9958  return Br;
9959 }

◆ BrHWW4fRatio()

double NPSMEFTd6::BrHWW4fRatio ( ) const
virtual

The ratio of the Br \((H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model.

Returns
Br \((H\to WW^*\to 4f)\)/Br \((H\to WW^*\to 4f)_{\mathrm{SM}}\)

Definition at line 10037 of file NPSMEFTd6.cpp.

10038 {
10039  double Br = 1.0;
10040  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10041 
10042  dGHiR1= deltaGammaHWW4fRatio1();
10043 
10044  Br += dGHiR1 - dGammaHTotR1;
10045 
10046  if (FlagQuadraticTerms) {
10047 
10048  dGHiR2= deltaGammaHWW4fRatio2();
10049 
10050  //Add contributions that are quadratic in the effective coefficients
10051  Br += - dGHiR1 * dGammaHTotR1
10052  + dGHiR2 - dGammaHTotR2
10053  + pow(dGammaHTotR1,2.0);
10054  }
10055 
10056  GHiR += dGHiR1 + dGHiR2;
10057  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10058 
10059  return Br;
10060 }

◆ BrHWW4jRatio()

double NPSMEFTd6::BrHWW4jRatio ( ) const
virtual

The ratio of the Br \((H\to WW^*\to 4j)\) in the current model and in the Standard Model.

Returns
Br \((H\to WW^*\to 4j)\)/Br \((H\to WW^*\to 4j)_{\mathrm{SM}}\)

Definition at line 9986 of file NPSMEFTd6.cpp.

9987 {
9988  double Br = 1.0;
9989  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
9990 
9991  dGHiR1= deltaGammaHWW4jRatio1();
9992 
9993  Br += dGHiR1 - dGammaHTotR1;
9994 
9995  if (FlagQuadraticTerms) {
9996 
9997  dGHiR2= deltaGammaHWW4jRatio2();
9998 
9999  //Add contributions that are quadratic in the effective coefficients
10000  Br += - dGHiR1 * dGammaHTotR1
10001  + dGHiR2 - dGammaHTotR2
10002  + pow(dGammaHTotR1,2.0);
10003  }
10004 
10005  GHiR += dGHiR1 + dGHiR2;
10006  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10007 
10008  return Br;
10009 }

◆ BrHWWRatio()

double NPSMEFTd6::BrHWWRatio ( ) const
virtual

The ratio of the Br \((H\to WW)\) in the current model and in the Standard Model.

Returns
Br \((H\to WW)\)/Br \((H\to WW)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 9904 of file NPSMEFTd6.cpp.

9905 {
9906 
9907  return BrHWW4fRatio();
9908 
9909 }

◆ BrHZddRatio()

double NPSMEFTd6::BrHZddRatio ( ) const
virtual

The ratio of the Br \((H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model.

Returns
Br \((H\to Z d d)\)/Br \((H\to Z d d)_{\mathrm{SM}}\)

Definition at line 10282 of file NPSMEFTd6.cpp.

10283 {
10284  double Br = 1.0;
10285  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10286 
10287  dGHiR1= deltaGammaHZddRatio1();
10288 
10289  Br += dGHiR1 - dGammaHTotR1;
10290 
10291  if (FlagQuadraticTerms) {
10292 
10293  dGHiR2= deltaGammaHZddRatio2();
10294 
10295  //Add contributions that are quadratic in the effective coefficients
10296  Br += - dGHiR1 * dGammaHTotR1
10297  + dGHiR2 - dGammaHTotR2
10298  + pow(dGammaHTotR1,2.0);
10299  }
10300 
10301  GHiR += dGHiR1 + dGHiR2;
10302  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10303 
10304  return Br;
10305 }

◆ BrHZffRatio()

double NPSMEFTd6::BrHZffRatio ( ) const
virtual

The ratio of the Br \((H\to Zff)\), with \(f\) any fermion, in the current model and in the Standard Model.

Returns
Br \((H\to Zff)\)/Br \((H\to Zff)_{\mathrm{SM}}\)

Definition at line 10325 of file NPSMEFTd6.cpp.

10326 {
10327  double Br = 1.0;
10328  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10329 
10330  dGHiR1= deltaGammaHZffRatio1();
10331 
10332  Br += dGHiR1 - dGammaHTotR1;
10333 
10334  if (FlagQuadraticTerms) {
10335 
10336  dGHiR2= deltaGammaHZffRatio2();
10337 
10338  //Add contributions that are quadratic in the effective coefficients
10339  Br += - dGHiR1 * dGammaHTotR1
10340  + dGHiR2 - dGammaHTotR2
10341  + pow(dGammaHTotR1,2.0);
10342  }
10343 
10344  GHiR += dGHiR1 + dGHiR2;
10345  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10346 
10347  return Br;
10348 }

◆ BrHZgaeeRatio()

double NPSMEFTd6::BrHZgaeeRatio ( ) const
virtual

The ratio of the Br \((H\to Z\gamma\to ee\gamma)\) in the current model and in the Standard Model.

Returns
Br \((H\to Z\gamma\to ee\gamma)\)/Br \((H\to Z\gamma\to ee\gamma)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10416 of file NPSMEFTd6.cpp.

10417 {
10418  double deltaBRratio;
10419 
10420  deltaBRratio = deltaGamma_Zf(leptons[ELECTRON]) / (trueSM.GammaZ(leptons[ELECTRON]));
10421 
10422  deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
10423 
10424  return ( BrHZgaRatio() + deltaBRratio );
10425 }

◆ BrHZgallRatio()

double NPSMEFTd6::BrHZgallRatio ( ) const
virtual

The ratio of the Br \((H\to Z\gamma\to ll\gamma)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.

Returns
Br \((H\to Z\gamma\to ll\gamma)\)/Br \((H\to Z\gamma\to ll\gamma)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10401 of file NPSMEFTd6.cpp.

10402 {
10403  double deltaBRratio;
10404 
10405  deltaBRratio = deltaGamma_Zf(leptons[ELECTRON])
10406  + deltaGamma_Zf(leptons[MU]);
10407 
10408  deltaBRratio = deltaBRratio /
10410 
10411  deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
10412 
10413  return ( BrHZgaRatio() + deltaBRratio );
10414 }

◆ BrHZgamumuRatio()

double NPSMEFTd6::BrHZgamumuRatio ( ) const
virtual

The ratio of the Br \((H\to Z\gamma\to \mu\mu\gamma)\) in the current model and in the Standard Model.

Returns
Br \((H\to Z\gamma\to \mu\mu\gamma)\)/Br \((H\to Z\gamma\to \mu\mu\gamma)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10427 of file NPSMEFTd6.cpp.

10428 {
10429  double deltaBRratio;
10430 
10431  deltaBRratio = deltaGamma_Zf(leptons[MU])/(trueSM.GammaZ(leptons[MU]));
10432 
10433  deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
10434 
10435  return ( BrHZgaRatio() + deltaBRratio );
10436 }

◆ BrHZgaRatio()

double NPSMEFTd6::BrHZgaRatio ( ) const
virtual

The ratio of the Br \((H\to Z\gamma)\) in the current model and in the Standard Model.

Returns
Br \((H\to Z\gamma)\)/Br \((H\to Z\gamma)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10375 of file NPSMEFTd6.cpp.

10376 {
10377  double Br = 1.0;
10378  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10379 
10380  dGHiR1= deltaGammaHZgaRatio1();
10381 
10382  Br += dGHiR1 - dGammaHTotR1;
10383 
10384  if (FlagQuadraticTerms) {
10385 
10386  dGHiR2= deltaGammaHZgaRatio2();
10387 
10388  //Add contributions that are quadratic in the effective coefficients
10389  Br += - dGHiR1 * dGammaHTotR1
10390  + dGHiR2 - dGammaHTotR2
10391  + pow(dGammaHTotR1,2.0);
10392  }
10393 
10394  GHiR += dGHiR1 + dGHiR2;
10395  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10396 
10397  return Br;
10398 
10399 }

◆ BrHZllRatio()

double NPSMEFTd6::BrHZllRatio ( ) const
virtual

The ratio of the Br \((H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.

Returns
Br \((H\to Zll)\)/Br \((H\to Zll)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10067 of file NPSMEFTd6.cpp.

10068 {
10069  double Br = 1.0;
10070  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10071 
10072  dGHiR1= deltaGammaHZllRatio1();
10073 
10074  Br += dGHiR1 - dGammaHTotR1;
10075 
10076  if (FlagQuadraticTerms) {
10077 
10078  dGHiR2= deltaGammaHZllRatio2();
10079 
10080  //Add contributions that are quadratic in the effective coefficients
10081  Br += - dGHiR1 * dGammaHTotR1
10082  + dGHiR2 - dGammaHTotR2
10083  + pow(dGammaHTotR1,2.0);
10084  }
10085 
10086  GHiR += dGHiR1 + dGHiR2;
10087  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10088 
10089  return Br;
10090 }

◆ BrHZuuRatio()

double NPSMEFTd6::BrHZuuRatio ( ) const
virtual

The ratio of the Br \((H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model.

Returns
Br \((H\to Z u u)\)/Br \((H\to Z u u)_{\mathrm{SM}}\)

Definition at line 10242 of file NPSMEFTd6.cpp.

10243 {
10244  double Br = 1.0;
10245  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10246 
10247  dGHiR1= deltaGammaHZuuRatio1();
10248 
10249  Br += dGHiR1 - dGammaHTotR1;
10250 
10251  if (FlagQuadraticTerms) {
10252 
10253  dGHiR2= deltaGammaHZuuRatio2();
10254 
10255  //Add contributions that are quadratic in the effective coefficients
10256  Br += - dGHiR1 * dGammaHTotR1
10257  + dGHiR2 - dGammaHTotR2
10258  + pow(dGammaHTotR1,2.0);
10259  }
10260 
10261  GHiR += dGHiR1 + dGHiR2;
10262  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10263 
10264  return Br;
10265 }

◆ BrHZvvRatio()

double NPSMEFTd6::BrHZvvRatio ( ) const
virtual

The ratio of the Br \((H\to Z\nu\nu)\) in the current model and in the Standard Model.

Returns
Br \((H\to Z\nu\nu)\)/Br \((H\to Z\nu\nu)_{\mathrm{SM}}\)

Definition at line 10192 of file NPSMEFTd6.cpp.

10193 {
10194  double Br = 1.0;
10195  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10196 
10197  dGHiR1= deltaGammaHZvvRatio1();
10198 
10199  Br += dGHiR1 - dGammaHTotR1;
10200 
10201  if (FlagQuadraticTerms) {
10202 
10203  dGHiR2= deltaGammaHZvvRatio2();
10204 
10205  //Add contributions that are quadratic in the effective coefficients
10206  Br += - dGHiR1 * dGammaHTotR1
10207  + dGHiR2 - dGammaHTotR2
10208  + pow(dGammaHTotR1,2.0);
10209  }
10210 
10211  GHiR += dGHiR1 + dGHiR2;
10212  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10213 
10214  return Br;
10215 }

◆ BrHZZ2e2muRatio()

double NPSMEFTd6::BrHZZ2e2muRatio ( ) const
virtual

The ratio of the Br \((H\to ZZ* \to 2e 2\mu)\) in the current model and in the Standard Model.

Returns
Br \((H\to ZZ* \to 2e 2\mu)\)/Br \((H\to ZZ* \to 2e 2\mu)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10142 of file NPSMEFTd6.cpp.

10143 {
10144  double Br = 1.0;
10145  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10146 
10147  dGHiR1= deltaGammaHZZ2e2muRatio1();
10148 
10149  Br += dGHiR1 - dGammaHTotR1;
10150 
10151  if (FlagQuadraticTerms) {
10152 
10153  dGHiR2= deltaGammaHZZ2e2muRatio2();
10154 
10155  //Add contributions that are quadratic in the effective coefficients
10156  Br += - dGHiR1 * dGammaHTotR1
10157  + dGHiR2 - dGammaHTotR2
10158  + pow(dGammaHTotR1,2.0);
10159  }
10160 
10161  GHiR += dGHiR1 + dGHiR2;
10162  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10163 
10164  return Br;
10165 }

◆ BrHZZ4dRatio()

double NPSMEFTd6::BrHZZ4dRatio ( ) const
virtual

The ratio of the Br \((H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model.

Returns
Br \((H\to ZZ* \to 4 d)\)/Br \((H\to ZZ* \to 4 d)_{\mathrm{SM}}\)

Definition at line 10307 of file NPSMEFTd6.cpp.

10308 {
10309  double deltaBRratio;
10310 
10311  deltaBRratio = deltaGamma_Zf(quarks[DOWN])
10314 
10315  deltaBRratio = deltaBRratio /
10316  ( trueSM.GammaZ(quarks[DOWN])
10318  + trueSM.GammaZ(quarks[BOTTOM]) );
10319 
10320  deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
10321 
10322  return ( BrHZddRatio() + deltaBRratio );
10323 }

◆ BrHZZ4eRatio()

double NPSMEFTd6::BrHZZ4eRatio ( ) const
virtual

The ratio of the Br \((H\to ZZ* \to 4e)\) in the current model and in the Standard Model.

Returns
Br \((H\to ZZ* \to 4e)\)/Br \((H\to ZZ* \to 4e)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10117 of file NPSMEFTd6.cpp.

10118 {
10119  double Br = 1.0;
10120  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10121 
10122  dGHiR1= deltaGammaHZZ4eRatio1();
10123 
10124  Br += dGHiR1 - dGammaHTotR1;
10125 
10126  if (FlagQuadraticTerms) {
10127 
10128  dGHiR2= deltaGammaHZZ4eRatio2();
10129 
10130  //Add contributions that are quadratic in the effective coefficients
10131  Br += - dGHiR1 * dGammaHTotR1
10132  + dGHiR2 - dGammaHTotR2
10133  + pow(dGammaHTotR1,2.0);
10134  }
10135 
10136  GHiR += dGHiR1 + dGHiR2;
10137  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10138 
10139  return Br;
10140 }

◆ BrHZZ4fRatio()

double NPSMEFTd6::BrHZZ4fRatio ( ) const
virtual

The ratio of the Br \((H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model.

Returns
Br \((H\to ZZ* \to 4f)\)/Br \((H\to ZZ* \to 4f)_{\mathrm{SM}}\)

Definition at line 10350 of file NPSMEFTd6.cpp.

10351 {
10352  double Br = 1.0;
10353  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10354 
10355  dGHiR1= deltaGammaHZZ4fRatio1();
10356 
10357  Br += dGHiR1 - dGammaHTotR1;
10358 
10359  if (FlagQuadraticTerms) {
10360 
10361  dGHiR2= deltaGammaHZZ4fRatio2();
10362 
10363  //Add contributions that are quadratic in the effective coefficients
10364  Br += - dGHiR1 * dGammaHTotR1
10365  + dGHiR2 - dGammaHTotR2
10366  + pow(dGammaHTotR1,2.0);
10367  }
10368 
10369  GHiR += dGHiR1 + dGHiR2;
10370  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10371 
10372  return Br;
10373 }

◆ BrHZZ4lRatio()

double NPSMEFTd6::BrHZZ4lRatio ( ) const
virtual

The ratio of the Br \((H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.

Returns
Br \((H\to ZZ* \to 4l)\)/Br \((H\to ZZ* \to 4l)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10092 of file NPSMEFTd6.cpp.

10093 {
10094  double Br = 1.0;
10095  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10096 
10097  dGHiR1= deltaGammaHZZ4lRatio1();
10098 
10099  Br += dGHiR1 - dGammaHTotR1;
10100 
10101  if (FlagQuadraticTerms) {
10102 
10103  dGHiR2= deltaGammaHZZ4lRatio2();
10104 
10105  //Add contributions that are quadratic in the effective coefficients
10106  Br += - dGHiR1 * dGammaHTotR1
10107  + dGHiR2 - dGammaHTotR2
10108  + pow(dGammaHTotR1,2.0);
10109  }
10110 
10111  GHiR += dGHiR1 + dGHiR2;
10112  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10113 
10114  return Br;
10115 }

◆ BrHZZ4muRatio()

double NPSMEFTd6::BrHZZ4muRatio ( ) const
virtual

The ratio of the Br \((H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model.

Returns
Br \((H\to ZZ* \to 4\mu)\)/Br \((H\to ZZ* \to 4\mu)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10167 of file NPSMEFTd6.cpp.

10168 {
10169  double Br = 1.0;
10170  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10171 
10172  dGHiR1= deltaGammaHZZ4muRatio1();
10173 
10174  Br += dGHiR1 - dGammaHTotR1;
10175 
10176  if (FlagQuadraticTerms) {
10177 
10178  dGHiR2= deltaGammaHZZ4muRatio2();
10179 
10180  //Add contributions that are quadratic in the effective coefficients
10181  Br += - dGHiR1 * dGammaHTotR1
10182  + dGHiR2 - dGammaHTotR2
10183  + pow(dGammaHTotR1,2.0);
10184  }
10185 
10186  GHiR += dGHiR1 + dGHiR2;
10187  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10188 
10189  return Br;
10190 }

◆ BrHZZ4uRatio()

double NPSMEFTd6::BrHZZ4uRatio ( ) const
virtual

The ratio of the Br \((H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model.

Returns
Br \((H\to ZZ* \to 4 u)\)/Br \((H\to ZZ* \to 4 u)_{\mathrm{SM}}\)

Definition at line 10267 of file NPSMEFTd6.cpp.

10268 {
10269  double deltaBRratio;
10270 
10271  deltaBRratio = deltaGamma_Zf(quarks[UP])
10273 
10274  deltaBRratio = deltaBRratio /
10276 
10277  deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
10278 
10279  return ( BrHZuuRatio() + deltaBRratio );
10280 }

◆ BrHZZ4vRatio()

double NPSMEFTd6::BrHZZ4vRatio ( ) const
virtual

The ratio of the Br \((H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model.

Returns
Br \((H\to ZZ* \to 4\nu)\)/Br \((H\to ZZ* \to 4\nu)_{\mathrm{SM}}\)

Definition at line 10217 of file NPSMEFTd6.cpp.

10218 {
10219  double Br = 1.0;
10220  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10221 
10222  dGHiR1= deltaGammaHZZ4vRatio1();
10223 
10224  Br += dGHiR1 - dGammaHTotR1;
10225 
10226  if (FlagQuadraticTerms) {
10227 
10228  dGHiR2= deltaGammaHZZ4vRatio2();
10229 
10230  //Add contributions that are quadratic in the effective coefficients
10231  Br += - dGHiR1 * dGammaHTotR1
10232  + dGHiR2 - dGammaHTotR2
10233  + pow(dGammaHTotR1,2.0);
10234  }
10235 
10236  GHiR += dGHiR1 + dGHiR2;
10237  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10238 
10239  return Br;
10240 }

◆ BrHZZRatio()

double NPSMEFTd6::BrHZZRatio ( ) const
virtual

The ratio of the Br \((H\to ZZ)\) in the current model and in the Standard Model.

Returns
Br \((H\to ZZ)\)/Br \((H\to ZZ)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10062 of file NPSMEFTd6.cpp.

10063 {
10064  return BrHZZ4fRatio();
10065 }

◆ CfB_diag()

gslpp::complex NPSMEFTd6::CfB_diag ( const Particle  f) const
protected

The diagonal entry of the dimension-6 operator coefficient \(C_{EB,UB,DB}\) corresponding to particle f.

Parameters
[in]fa lepton or quark
Returns
\((\)C_{fB})_{ff} \(\)

Definition at line 2569 of file NPSMEFTd6.cpp.

2570 {
2571  if (f.is("NEUTRINO_1") || f.is("NEUTRINO_2") || f.is("NEUTRINO_3"))
2572  return 0.0;
2573  else if (f.is("ELECTRON"))
2574  return 0.0;
2575  else if (f.is("MU"))
2576  return 0.0;
2577  else if (f.is("TAU"))
2578  return 0.0;
2579  else if (f.is("UP"))
2580  return gslpp::complex(CiuB_11r, CuB_11i, false);
2581  else if (f.is("CHARM"))
2582  return gslpp::complex(CiuB_22r, CuB_22i, false);
2583  else if (f.is("TOP"))
2584  return gslpp::complex(CiuB_33r, CuB_33i, false);
2585  else if (f.is("DOWN"))
2586  return 0.0;
2587  else if (f.is("STRANGE"))
2588  return 0.0;
2589  else if (f.is("BOTTOM"))
2590  return 0.0;
2591  else
2592  throw std::runtime_error("NPSMEFTd6::CfB_diag(): wrong argument");
2593 }

◆ CfG_diag()

gslpp::complex NPSMEFTd6::CfG_diag ( const Particle  f) const
protected

The diagonal entry of the dimension-6 operator coefficient \(C_{UG,DG}\) corresponding to particle f.

Parameters
[in]fa lepton or quark
Returns
\((\)C_{fG})_{ff} \(\)

Definition at line 2517 of file NPSMEFTd6.cpp.

2518 {
2519  if (f.is("NEUTRINO_1") || f.is("NEUTRINO_2") || f.is("NEUTRINO_3"))
2520  return 0.0;
2521  else if (f.is("ELECTRON"))
2522  return 0.0;
2523  else if (f.is("MU"))
2524  return 0.0;
2525  else if (f.is("TAU"))
2526  return 0.0;
2527  else if (f.is("UP"))
2528  return gslpp::complex(CiuG_11r, CuG_11i, false);
2529  else if (f.is("CHARM"))
2530  return gslpp::complex(CiuG_22r, CuG_22i, false);
2531  else if (f.is("TOP"))
2532  return gslpp::complex(CiuG_33r, CuG_33i, false);
2533  else if (f.is("DOWN"))
2534  return 0.0;
2535  else if (f.is("STRANGE"))
2536  return 0.0;
2537  else if (f.is("BOTTOM"))
2538  return 0.0;
2539  else
2540  throw std::runtime_error("NPSMEFTd6::CfG_diag(): wrong argument");
2541 }

◆ CfH_diag()

gslpp::complex NPSMEFTd6::CfH_diag ( const Particle  f) const
protected

The diagonal entry of the dimension-6 operator coefficient \(C_{EH,UH,DH}\) corresponding to particle f.

Parameters
[in]fa lepton or quark
Returns
\((\)C_{fH})_{ff} \(\)

Definition at line 2491 of file NPSMEFTd6.cpp.

2492 {
2493  if (f.is("NEUTRINO_1") || f.is("NEUTRINO_2") || f.is("NEUTRINO_3"))
2494  return 0.0;
2495  else if (f.is("ELECTRON"))
2496  return gslpp::complex(CieH_11r, CeH_11i, false);
2497  else if (f.is("MU"))
2498  return gslpp::complex(CieH_22r, CeH_22i, false);
2499  else if (f.is("TAU"))
2500  return gslpp::complex(CieH_33r, CeH_33i, false);
2501  else if (f.is("UP"))
2502  return gslpp::complex(CiuH_11r, CuH_11i, false);
2503  else if (f.is("CHARM"))
2504  return gslpp::complex(CiuH_22r, CuH_22i, false);
2505  else if (f.is("TOP"))
2506  return gslpp::complex(CiuH_33r, CuH_33i, false);
2507  else if (f.is("DOWN"))
2508  return gslpp::complex(CidH_11r, CdH_11i, false);
2509  else if (f.is("STRANGE"))
2510  return gslpp::complex(CidH_22r, CdH_22i, false);
2511  else if (f.is("BOTTOM"))
2512  return gslpp::complex(CidH_33r, CdH_33i, false);
2513  else
2514  throw std::runtime_error("NPSMEFTd6::CfH_diag(): wrong argument");
2515 }

◆ CfW_diag()

gslpp::complex NPSMEFTd6::CfW_diag ( const Particle  f) const
protected

The diagonal entry of the dimension-6 operator coefficient \(C_{EW,UW,DW}\) corresponding to particle f.

Parameters
[in]fa lepton or quark
Returns
\((\)C_{fW})_{ff} \(\)

Definition at line 2543 of file NPSMEFTd6.cpp.

2544 {
2545  if (f.is("NEUTRINO_1") || f.is("NEUTRINO_2") || f.is("NEUTRINO_3"))
2546  return 0.0;
2547  else if (f.is("ELECTRON"))
2548  return 0.0;
2549  else if (f.is("MU"))
2550  return 0.0;
2551  else if (f.is("TAU"))
2552  return 0.0;
2553  else if (f.is("UP"))
2554  return gslpp::complex(CiuW_11r, CuW_11i, false);
2555  else if (f.is("CHARM"))
2556  return gslpp::complex(CiuW_22r, CuW_22i, false);
2557  else if (f.is("TOP"))
2558  return gslpp::complex(CiuW_33r, CuW_33i, false);
2559  else if (f.is("DOWN"))
2560  return 0.0;
2561  else if (f.is("STRANGE"))
2562  return 0.0;
2563  else if (f.is("BOTTOM"))
2564  return 0.0;
2565  else
2566  throw std::runtime_error("NPSMEFTd6::CfW_diag(): wrong argument");
2567 }

◆ cgaga_HB()

double NPSMEFTd6::cgaga_HB ( ) const
virtual

The Higgs-basis coupling \(c_{\gamma\gamma}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(c_{\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 15246 of file NPSMEFTd6.cpp.

15247 {
15248  double ciHB;
15249 
15251 
15252  return ciHB;
15253 }

◆ cgg_HB()

double NPSMEFTd6::cgg_HB ( ) const
virtual

The Higgs-basis coupling \(c_{gg}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(c_{gg}\)

Reimplemented from NPbase.

Definition at line 15256 of file NPSMEFTd6.cpp.

15257 {
15258  double ciHB;
15259 
15260  ciHB = (1.0/(M_PI * AlsMz))*CHG*v2_over_LambdaNP2;
15261 
15262  return ciHB;
15263 }

◆ cggEff_HB()

double NPSMEFTd6::cggEff_HB ( ) const
virtual

The effective Higgs-basis coupling \(c_{gg}^{Eff}\). (Similar to cgg_HB but including modifications of SM loops.) (See arXiv: 1505.00046 [hep-ph] document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(c_{gg}^{Eff}\)

Reimplemented from NPbase.

Definition at line 15265 of file NPSMEFTd6.cpp.

15266 {
15267  double ciHB;
15268 
15269  double m_t = mtpole;
15270  //doulbe m_t = quarks[TOP].getMass();
15271  double m_b = quarks[BOTTOM].getMass();
15272  double m_c = quarks[CHARM].getMass();
15273 
15274  double At = deltayt_HB() * AH_f(4.0 * m_t * m_t / mHl / mHl).real();
15275  double Ab = deltayb_HB() * AH_f(4.0 * m_b * m_b / mHl / mHl).real();
15276  double Ac = deltayc_HB() * AH_f(4.0 * m_c * m_c / mHl / mHl).real();
15277 
15278  ciHB = cgg_HB() + (1.0/16.0/M_PI/M_PI) * (At + Ab + Ac) ;
15279 
15280  return ciHB;
15281 }

◆ CheckParameters()

bool NPSMEFTd6::CheckParameters ( const std::map< std::string, double > &  DPars)
virtual

A method to check if all the mandatory parameters for NPSMEFTd6 have been provided in model initialization.

Parameters
[in]DParsa map of the parameters that are being updated in the Monte Carlo run (including parameters that are varied and those that are held constant)
Returns
a boolean that is true if the execution is successful

Reimplemented from StandardModel.

Definition at line 2328 of file NPSMEFTd6.cpp.

2329 {
2331  if (FlagRotateCHWCHB) {
2332  for (int i = 0; i < NNPSMEFTd6Vars_LFU_QFU; i++) {
2333  if (DPars.find(NPSMEFTd6VarsRot_LFU_QFU[i]) == DPars.end()) {
2334  std::cout << "ERROR: Missing mandatory NPSMEFTd6_LFU_QFU parameter "
2335  << NPSMEFTd6VarsRot_LFU_QFU[i] << std::endl;
2338  }
2339  }
2340  } else {
2341  for (int i = 0; i < NNPSMEFTd6Vars_LFU_QFU; i++) {
2342  if (DPars.find(NPSMEFTd6Vars_LFU_QFU[i]) == DPars.end()) {
2343  std::cout << "ERROR: Missing mandatory NPSMEFTd6_LFU_QFU parameter "
2344  << NPSMEFTd6Vars_LFU_QFU[i] << std::endl;
2347  }
2348  }
2349  }
2350  } else if (!FlagLeptonUniversal && !FlagQuarkUniversal) {
2351  if (FlagRotateCHWCHB) {
2352  for (int i = 0; i < NNPSMEFTd6Vars; i++) {
2353  if (DPars.find(NPSMEFTd6VarsRot[i]) == DPars.end()) {
2354  std::cout << "ERROR: Missing mandatory NPSMEFTd6 parameter "
2355  << NPSMEFTd6VarsRot[i] << std::endl;
2358  }
2359  }
2360  } else {
2361  for (int i = 0; i < NNPSMEFTd6Vars; i++) {
2362  if (DPars.find(NPSMEFTd6Vars[i]) == DPars.end()) {
2363  std::cout << "ERROR: Missing mandatory NPSMEFTd6 parameter "
2364  << NPSMEFTd6Vars[i] << std::endl;
2367  }
2368  }
2369  }
2370 
2371  } else
2372  throw std::runtime_error("Error in NPSMEFTd6::CheckParameters()");
2373 
2374  return (NPbase::CheckParameters(DPars));
2375 }

◆ CHF1_diag()

double NPSMEFTd6::CHF1_diag ( const Particle  F) const
protected

The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(1)}\) corresponding to particle F.

Parameters
[in]Fa lepton or quark
Returns
\((\)C_{HF}^{(1)})_{FF} \(\)

Definition at line 2414 of file NPSMEFTd6.cpp.

2415 {
2416  if (F.is("NEUTRINO_1") || F.is("ELECTRON"))
2417  return CiHL1_11;
2418  else if (F.is("NEUTRINO_2") || F.is("MU"))
2419  return CiHL1_22;
2420  else if (F.is("NEUTRINO_3") || F.is("TAU"))
2421  return CiHL1_33;
2422  else if (F.is("UP") || F.is("DOWN"))
2423  return CiHQ1_11;
2424  else if (F.is("CHARM") || F.is("STRANGE"))
2425  return CiHQ1_22;
2426  else if (F.is("TOP") || F.is("BOTTOM"))
2427  return CiHQ1_33;
2428  else
2429  throw std::runtime_error("NPSMEFTd6::CHF1_diag(): wrong argument");
2430 }

◆ CHF3_diag()

double NPSMEFTd6::CHF3_diag ( const Particle  F) const
protected

The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(3)}\) corresponding to particle F.

Parameters
[in]Fa lepton or quark
Returns
\((\)C_{HF}^{(3)})_{FF} \(\)

Definition at line 2432 of file NPSMEFTd6.cpp.

2433 {
2434  if (F.is("NEUTRINO_1") || F.is("ELECTRON"))
2435  return CiHL3_11;
2436  else if (F.is("NEUTRINO_2") || F.is("MU"))
2437  return CiHL3_22;
2438  else if (F.is("NEUTRINO_3") || F.is("TAU"))
2439  return CiHL3_33;
2440  else if (F.is("UP") || F.is("DOWN"))
2441  return CiHQ3_11;
2442  else if (F.is("CHARM") || F.is("STRANGE"))
2443  return CiHQ3_22;
2444  else if (F.is("TOP") || F.is("BOTTOM"))
2445  return CiHQ3_33;
2446  else
2447  throw std::runtime_error("NPSMEFTd6::CHF3_diag(): wrong argument");
2448 }

◆ CHf_diag()

double NPSMEFTd6::CHf_diag ( const Particle  f) const
protected

The diagonal entry of the dimension-6 operator coefficient \(C_{HE,HU,HD}\) corresponding to particle f.

Parameters
[in]fa lepton or quark
Returns
\((\)C_{Hf})_{ff} \(\)

Definition at line 2450 of file NPSMEFTd6.cpp.

2451 {
2452  if (f.is("NEUTRINO_1") || f.is("NEUTRINO_2") || f.is("NEUTRINO_3"))
2453  return 0.0;
2454  else if (f.is("ELECTRON"))
2455  return CiHe_11;
2456  else if (f.is("MU"))
2457  return CiHe_22;
2458  else if (f.is("TAU"))
2459  return CiHe_33;
2460  else if (f.is("UP"))
2461  return CiHu_11;
2462  else if (f.is("CHARM"))
2463  return CiHu_22;
2464  else if (f.is("TOP"))
2465  return CiHu_33;
2466  else if (f.is("DOWN"))
2467  return CiHd_11;
2468  else if (f.is("STRANGE"))
2469  return CiHd_22;
2470  else if (f.is("BOTTOM"))
2471  return CiHd_33;
2472  else
2473  throw std::runtime_error("NPSMEFTd6::CHf_diag(): wrong argument");
2474 }

◆ CHud_diag()

gslpp::complex NPSMEFTd6::CHud_diag ( const Particle  u) const
protected

The diagonal entry of the dimension-6 operator coefficient \(C_{Hud}\) corresponding to particle f.

Parameters
[in]ua quark
Returns
\((\)C_{Hud})_{ud} \(\)

Definition at line 2476 of file NPSMEFTd6.cpp.

2477 {
2478  if (!u.is("QUARK") || u.getIndex() % 2 != 0)
2479  throw std::runtime_error("NPSMEFTd6::CHud_diag(): wrong argument");
2480 
2481  if (u.is("UP"))
2482  return gslpp::complex(CHud_11r, CHud_11i, false);
2483  else if (u.is("CHARM"))
2484  return gslpp::complex(CHud_22r, CHud_22i, false);
2485  else if (u.is("TOP"))
2486  return gslpp::complex(CHud_22r, CHud_33i, false);
2487  else
2488  throw std::runtime_error("NPSMEFTd6::CHud_diag(): wrong argument");
2489 }

◆ CLL_bottom()

double NPSMEFTd6::CLL_bottom ( ) const

Definition at line 16170 of file NPSMEFTd6.cpp.

16171 {
16173 }

◆ CLL_charm()

double NPSMEFTd6::CLL_charm ( ) const

Definition at line 16160 of file NPSMEFTd6.cpp.

16161 {
16163 }

◆ CLL_down()

double NPSMEFTd6::CLL_down ( ) const

Definition at line 16155 of file NPSMEFTd6.cpp.

16156 {
16157  return (CLQ1_1111+CLQ3_1111);
16158 }

◆ CLL_mu()

double NPSMEFTd6::CLL_mu ( ) const

Definition at line 16140 of file NPSMEFTd6.cpp.

16141 {
16142  return (CLL_1122 + CLL_2211 + CiLL_1221 + CiLL_2112);
16143 }

◆ CLL_strange()

double NPSMEFTd6::CLL_strange ( ) const

Definition at line 16165 of file NPSMEFTd6.cpp.

16166 {
16168 }

◆ CLL_tau()

double NPSMEFTd6::CLL_tau ( ) const

Definition at line 16145 of file NPSMEFTd6.cpp.

16146 {
16147  return (CLL_1133 + CLL_3311 + CLL_1331 + CLL_3113);
16148 }

◆ CLL_up()

double NPSMEFTd6::CLL_up ( ) const

Definition at line 16150 of file NPSMEFTd6.cpp.

16151 {
16152  return (CLQ1_1111-CLQ3_1111);
16153 }

◆ CLR_bottom()

double NPSMEFTd6::CLR_bottom ( ) const

Definition at line 16205 of file NPSMEFTd6.cpp.

16206 {
16207  return (CLd_1133+CLd_3311);
16208 }

◆ CLR_charm()

double NPSMEFTd6::CLR_charm ( ) const

Definition at line 16195 of file NPSMEFTd6.cpp.

16196 {
16197  return (CLu_1122+CLu_2211);
16198 }

◆ CLR_down()

double NPSMEFTd6::CLR_down ( ) const

Definition at line 16190 of file NPSMEFTd6.cpp.

16191 {
16192  return (CLd_1111);
16193 }

◆ CLR_mu()

double NPSMEFTd6::CLR_mu ( ) const

Definition at line 16175 of file NPSMEFTd6.cpp.

16176 {
16177  return (CLe_1122+CLe_2211);
16178 }

◆ CLR_strange()

double NPSMEFTd6::CLR_strange ( ) const

Definition at line 16200 of file NPSMEFTd6.cpp.

16201 {
16202  return (CLd_1122+CLd_2211);
16203 }

◆ CLR_tau()

double NPSMEFTd6::CLR_tau ( ) const

Definition at line 16180 of file NPSMEFTd6.cpp.

16181 {
16182  return (CLe_1133+CLe_3311);
16183 }

◆ CLR_up()

double NPSMEFTd6::CLR_up ( ) const

Definition at line 16185 of file NPSMEFTd6.cpp.

16186 {
16187  return (CLu_1111);
16188 }

◆ computeGammaTotalRatio()

double NPSMEFTd6::computeGammaTotalRatio ( ) const
virtual

The ratio of the \(\Gamma(H)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H)\)/ \(\Gamma(H)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10568 of file NPSMEFTd6.cpp.

10569 {
10570  double width = 1.0;
10571 
10572  width += dGammaHTotR1;
10573 
10574  if (FlagQuadraticTerms) {
10575  //Add contributions that are quadratic in the effective coefficients
10576  width += dGammaHTotR2;
10577  }
10578 
10579  if (width < 0) return std::numeric_limits<double>::quiet_NaN();
10580 
10581  return width;
10582 
10583 }

◆ CRL_bottom()

double NPSMEFTd6::CRL_bottom ( ) const

Definition at line 16240 of file NPSMEFTd6.cpp.

16241 {
16242  return (CQe_1133+CQe_3311);
16243 }

◆ CRL_charm()

double NPSMEFTd6::CRL_charm ( ) const

Definition at line 16230 of file NPSMEFTd6.cpp.

16231 {
16232  return (CQe_1122+CQe_2211);
16233 }

◆ CRL_down()

double NPSMEFTd6::CRL_down ( ) const

Definition at line 16225 of file NPSMEFTd6.cpp.

16226 {
16227  return (CQe_1111);
16228 }

◆ CRL_mu()

double NPSMEFTd6::CRL_mu ( ) const

Definition at line 16210 of file NPSMEFTd6.cpp.

16211 {
16212  return (CLe_1122+CLe_2211);
16213 }

◆ CRL_strange()

double NPSMEFTd6::CRL_strange ( ) const

Definition at line 16235 of file NPSMEFTd6.cpp.

16236 {
16237  return (CQe_1122+CQe_2211);
16238 }

◆ CRL_tau()

double NPSMEFTd6::CRL_tau ( ) const

Definition at line 16215 of file NPSMEFTd6.cpp.

16216 {
16217  return (CLe_1133+CLe_3311);
16218 }

◆ CRL_up()

double NPSMEFTd6::CRL_up ( ) const

Definition at line 16220 of file NPSMEFTd6.cpp.

16221 {
16222  return (CQe_1111);
16223 }

◆ CRR_bottom()

double NPSMEFTd6::CRR_bottom ( ) const

Definition at line 16276 of file NPSMEFTd6.cpp.

16277 {
16278  return (Ced_1133+Ced_3311);
16279 }

◆ CRR_charm()

double NPSMEFTd6::CRR_charm ( ) const

Definition at line 16266 of file NPSMEFTd6.cpp.

16267 {
16268  return (Ceu_1122+Ceu_2211);
16269 }

◆ CRR_down()

double NPSMEFTd6::CRR_down ( ) const

Definition at line 16261 of file NPSMEFTd6.cpp.

16262 {
16263  return (Ced_1111);
16264 }

◆ CRR_mu()

double NPSMEFTd6::CRR_mu ( ) const

Definition at line 16245 of file NPSMEFTd6.cpp.

16246 {
16247  return (Cee_1122+Cee_2211);
16248 }

◆ CRR_strange()

double NPSMEFTd6::CRR_strange ( ) const

Definition at line 16271 of file NPSMEFTd6.cpp.

16272 {
16273  return (Ced_1122+Ced_2211);
16274 }

◆ CRR_tau()

double NPSMEFTd6::CRR_tau ( ) const

Definition at line 16250 of file NPSMEFTd6.cpp.

16251 {
16252  return (Cee_1133+Cee_3311);
16253 }

◆ CRR_up()

double NPSMEFTd6::CRR_up ( ) const

Definition at line 16256 of file NPSMEFTd6.cpp.

16257 {
16258  return (Ceu_1111);
16259 }

◆ cZBox_HB()

double NPSMEFTd6::cZBox_HB ( ) const
virtual

The Higgs-basis coupling \(c_{z\Box}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(c_{z\Box}\)

Reimplemented from NPbase.

Definition at line 15210 of file NPSMEFTd6.cpp.

15211 {
15212  double ciHB;
15213 
15214  ciHB = (sW2_tree/eeMz2)*( DeltaGF() + 0.5*CiHD*v2_over_LambdaNP2 );
15215 
15216  ciHB = ciHB + 0.5*(sW2_tree/eeMz)*(CiDHB / cW_tree + CiDHW / sW_tree)*v2_over_LambdaNP2; // Extra, not in Warsaw basis
15217 
15218  return ciHB;
15219 }

◆ cZga_HB()

double NPSMEFTd6::cZga_HB ( ) const
virtual

The Higgs-basis coupling \(c_{z\gamma}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(c_{z\gamma}\)

Reimplemented from NPbase.

Definition at line 15234 of file NPSMEFTd6.cpp.

15235 {
15236  double ciHB;
15237 
15239 
15240  ciHB = ciHB + 0.5*(sW_tree*cW_tree/eeMz)*(CiDHB / sW_tree - CiDHW / cW_tree)*v2_over_LambdaNP2; // Extra, not in Warsaw basis
15241 
15242  return ciHB;
15243 }

◆ cZZ_HB()

double NPSMEFTd6::cZZ_HB ( ) const
virtual

The Higgs-basis coupling \(c_{zz}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(c_{zz}\)

Reimplemented from NPbase.

Definition at line 15222 of file NPSMEFTd6.cpp.

15223 {
15224  double ciHB;
15225 
15227 
15228  ciHB = ciHB - (sW2_tree*cW2_tree/eeMz)*(CiDHB / cW_tree + CiDHW / sW_tree)*v2_over_LambdaNP2; // Extra, not in Warsaw basis
15229 
15230  return ciHB;
15231 }

◆ deltaa0()

double NPSMEFTd6::deltaa0 ( ) const
virtual

The relative correction to the electromagnetic constant at zero momentum, \(\delta \alpha(0)/\alpha(0)\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\(\delta \alpha(0)/\alpha(0)\)

Definition at line 2718 of file NPSMEFTd6.cpp.

2719 {
2720  // Ref. value fixed in SM EW fit 2018: from PDG 2018
2721  return ( (aleMz - 0.0072973525664) / 0.0072973525664 );
2722 }

◆ deltaa02()

double NPSMEFTd6::deltaa02 ( ) const
virtual

The relative correction to the electromagnetic constant at zero momentum, \((\delta \alpha(0)/\alpha(0))^2\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\((\delta \alpha(0)/\alpha(0))^2\)

Definition at line 2724 of file NPSMEFTd6.cpp.

2725 {
2726  return ( 0.0 );
2727 }

◆ deltaaMZ()

double NPSMEFTd6::deltaaMZ ( ) const
virtual

The relative correction to the electromagnetic constant at the Z pole, \(\delta \alpha(M_Z^2)/\alpha(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\(\delta \alpha(M_Z^2)/\alpha(M_Z^2)\)

Definition at line 2707 of file NPSMEFTd6.cpp.

2708 {
2709  // Ref. value from SM EW fit 2018
2710  return ( (aleMz - 0.007754941997887603) / 0.007754941997887603 );
2711 }

◆ deltaaMZ2()

double NPSMEFTd6::deltaaMZ2 ( ) const
virtual

The relative correction to the electromagnetic constant at the Z pole, \((\delta \alpha(M_Z^2)/\alpha(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\((\delta \alpha(M_Z^2)/\alpha(M_Z^2))^2\)

Definition at line 2713 of file NPSMEFTd6.cpp.

2714 {
2715  return ( 0.0 );
2716 }

◆ deltaaSMZ()

double NPSMEFTd6::deltaaSMZ ( ) const
virtual

The relative correction to the strong coupling constant at the Z pole, \(\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\(\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2)\)

Definition at line 2729 of file NPSMEFTd6.cpp.

2730 {
2731  // Ref. value from SM EW fit 2018
2732  return ( (AlsMz - 0.1180) / 0.1180 );
2733 }

◆ deltaaSMZ2()

double NPSMEFTd6::deltaaSMZ2 ( ) const
virtual

The relative correction to the strong coupling constant at the Z pole, \((\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\((\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2))^2\)

Definition at line 2735 of file NPSMEFTd6.cpp.

2736 {
2737  return ( 0.0 );
2738 }

◆ deltacZ_HB()

double NPSMEFTd6::deltacZ_HB ( ) const
virtual

The Higgs-basis coupling \(\delta c_z\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(\delta c_z\)

Reimplemented from NPbase.

Definition at line 15200 of file NPSMEFTd6.cpp.

15201 {
15202  double ciHB;
15203 
15204  ciHB = delta_h - (3.0/2.0)*DeltaGF();
15205 
15206  return ciHB;
15207 }

◆ deltaG1_hWW()

double NPSMEFTd6::deltaG1_hWW ( ) const
virtual

The new physics contribution to the coupling of the effective interaction \(H W_{\mu\nu}^\dagger W^{\mu\nu}\).

Returns
\(\delta g_{HWW}^{(1)}\)

Reimplemented from NPbase.

Definition at line 2934 of file NPSMEFTd6.cpp.

2935 {
2936  return (( 2.0 * CiHW - sqrt( M_PI * aleMz ) * CiDHW / sW_tree ) * v2_over_LambdaNP2 / v());
2937 }

◆ deltaG1_hZA()

double NPSMEFTd6::deltaG1_hZA ( ) const
virtual

The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{\mu\nu}\).

Returns
\(\delta g_{HZA}^{(1)}\)

Reimplemented from NPbase.

Definition at line 2972 of file NPSMEFTd6.cpp.

2973 {
2974  return ( (delta_AZ + 0.5 * sqrt( M_PI * aleMz ) * (CiDHB / sW_tree - CiDHW / cW_tree) * v2_over_LambdaNP2 )/ v());
2975 }

◆ deltaG1_hZARatio()

double NPSMEFTd6::deltaG1_hZARatio ( ) const
virtual

The full new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.

Returns
\(\delta g_{HZA}^{(1)}/g_{HZA}^{(1),SM}\)

Reimplemented from NPbase.

Definition at line 2977 of file NPSMEFTd6.cpp.

2978 {
2979  double m_t = mtpole;
2980  double m_b = quarks[BOTTOM].getMass();
2981  double m_c = quarks[CHARM].getMass();
2982  double m_tau = leptons[TAU].getMass();
2983  double m_mu = leptons[MU].getMass();
2984 
2985  double M_w_2 = (trueSM.Mw())*(trueSM.Mw());
2986 
2987  double Qt = quarks[TOP].getCharge();
2988  double Qb = quarks[BOTTOM].getCharge();
2989  double Qc = quarks[CHARM].getCharge();
2990  double Qtau = leptons[TAU].getCharge();
2991  double Qmu = leptons[MU].getCharge();
2992 
2993  double tau_t = 4.0 * m_t * m_t / mHl / mHl;
2994  double tau_b = 4.0 * m_b * m_b / mHl / mHl;
2995  double tau_c = 4.0 * m_c * m_c / mHl / mHl;
2996  double tau_tau = 4.0 * m_tau * m_tau / mHl / mHl;
2997  double tau_mu = 4.0 * m_mu * m_mu / mHl / mHl;
2998  double tau_W = 4.0 * M_w_2 / mHl / mHl;
2999 
3000  double lambda_t = 4.0 * m_t * m_t / Mz / Mz;
3001  double lambda_b = 4.0 * m_b * m_b / Mz / Mz;
3002  double lambda_c = 4.0 * m_c * m_c / Mz / Mz;
3003  double lambda_tau = 4.0 * m_tau * m_tau / Mz / Mz;
3004  double lambda_mu = 4.0 * m_mu * m_mu / Mz / Mz;
3005  double lambda_W = 4.0 * M_w_2 / Mz / Mz;
3006  double alpha2 = sqrt(2.0)*GF*M_w_2 / M_PI;
3007  double aPiv = sqrt(ale*alpha2) / 4.0 / M_PI / v();
3008 
3009 // mod. of Higgs couplings
3010  gslpp::complex gSM, dg;
3011  gslpp::complex dKappa_t = cLHd6 * deltaG_hff(quarks[TOP]) / (-m_t / v());
3012  gslpp::complex dKappa_b = cLHd6 * deltaG_hff(quarks[BOTTOM]) / (-m_b / v());
3013  gslpp::complex dKappa_c = cLHd6 * deltaG_hff(quarks[CHARM]) / (-m_c / v());
3014  gslpp::complex dKappa_tau = cLHd6 * deltaG_hff(leptons[TAU]) / (-m_tau / v());
3015  gslpp::complex dKappa_mu = cLHd6 * deltaG_hff(leptons[MU]) / (-m_mu / v());
3016  double dKappa_W = cLHd6 * (0.5 * v() / M_w_2)*deltaG3_hWW();
3017 
3018 // mod of EW vector couplings vf =2 gvf
3019  double vSMt = 2.0*(quarks[TOP].getIsospin()) - 4.0 * Qt * sW2_tree;
3020  double vSMb = 2.0*(quarks[BOTTOM].getIsospin()) - 4.0 * Qb * sW2_tree;
3021  double vSMc = 2.0*(quarks[CHARM].getIsospin()) - 4.0 * Qc * sW2_tree;
3022  double vSMtau = 2.0*(leptons[TAU].getIsospin()) - 4.0 * Qtau * sW2_tree;
3023  double vSMmu = 2.0*(leptons[MU].getIsospin()) - 4.0 * Qmu * sW2_tree;
3024 
3025  double dvSMt = cLHd6 * 2.0*deltaGV_f(quarks[TOP]);
3026  double dvSMb = cLHd6 * 2.0*deltaGV_f(quarks[BOTTOM]);
3027  double dvSMc = cLHd6 * 2.0*deltaGV_f(quarks[CHARM]);
3028  double dvSMtau = cLHd6 * 2.0*deltaGV_f(leptons[TAU]);
3029  double dvSMmu = cLHd6 * 2.0*deltaGV_f(leptons[MU]);
3030 
3031  double deltaloc = deltaG1_hZA();
3032 
3033  gSM = -aPiv * ((3.0*vSMt*Qt*AHZga_f(tau_t,lambda_t) +
3034  3.0*vSMb*Qb*AHZga_f(tau_b,lambda_b) +
3035  3.0*vSMc*Qc*AHZga_f(tau_c,lambda_c) +
3036  vSMtau*Qtau*AHZga_f(tau_tau,lambda_tau)+
3037  vSMmu*Qmu*AHZga_f(tau_mu,lambda_mu))/cW_tree +
3038  AHZga_W(tau_W,lambda_W));
3039 
3040  dg = deltaloc/gSM - (aPiv/gSM) * (
3041  (3.0*vSMt*dKappa_t*Qt*AHZga_f(tau_t,lambda_t) +
3042  3.0*vSMb*dKappa_b*Qb*AHZga_f(tau_b,lambda_b) +
3043  3.0*vSMc*dKappa_c*Qc*AHZga_f(tau_c,lambda_c)+
3044  dKappa_tau*vSMtau*Qtau*AHZga_f(tau_tau,lambda_tau)+
3045  dKappa_mu*vSMmu*Qmu*AHZga_f(tau_mu,lambda_mu))/cW_tree +
3046  dKappa_W*AHZga_W(tau_W,lambda_W) +
3047  (3.0*dvSMt*Qt*AHZga_f(tau_t,lambda_t) +
3048  3.0*dvSMb*Qb*AHZga_f(tau_b,lambda_b) +
3049  3.0*dvSMc*Qc*AHZga_f(tau_c,lambda_c)+
3050  dvSMtau*Qtau*AHZga_f(tau_tau,lambda_tau)+
3051  dvSMmu*Qmu*AHZga_f(tau_mu,lambda_mu))/cW_tree
3052  );
3053 
3054  return dg.real();
3055 }

◆ deltaG1_hZZ()

double NPSMEFTd6::deltaG1_hZZ ( ) const
virtual

The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} Z^{\mu\nu}\).

Returns
\(\delta g_{HZZ}^{(1)}\)

Reimplemented from NPbase.

Definition at line 2955 of file NPSMEFTd6.cpp.

2956 {
2957  return ( (delta_ZZ - 0.5 * sqrt( M_PI * aleMz ) * (CiDHB / cW_tree + CiDHW / sW_tree) * v2_over_LambdaNP2 )/ v());
2958 }

◆ deltag1ZNP()

double NPSMEFTd6::deltag1ZNP ( ) const
virtual

The new physics contribution to the anomalous triple gauge coupling \(g_{1,Z}\).

Returns
\(\delta g_{1,Z}\)

Reimplemented from NPbase.

Definition at line 13495 of file NPSMEFTd6.cpp.

13496 {
13497  double NPdirect, NPindirect;
13498 
13499  /* From own calculations. Agrees with with LHCHXWG-INT-2015-001 for common interactions */
13500  NPdirect = sW_tree / sqrt( 4.0 * M_PI * aleMz );
13501  NPdirect = - NPdirect * (Mz * Mz / v () / v() ) * CiDHW * v2_over_LambdaNP2;
13502 
13503  NPindirect = - 1.0 / (cW2_tree-sW2_tree);
13504 
13505  NPindirect = NPindirect * (sW_tree * CiHWB / cW_tree
13506  + 0.25 * CiHD ) * v2_over_LambdaNP2
13507  + 0.5 * NPindirect * DeltaGF() ;
13508 
13509  return NPdirect + NPindirect + dg1Z ;
13510 }

◆ deltag1ZNPEff()

double NPSMEFTd6::deltag1ZNPEff ( ) const
virtual

The new physics contribution to the effective anomalous triple gauge coupling \(g_{1,Z}^{Eff}\) from arXiv: 1708.09079 [hep-ph].

Returns
\(\delta g_{1,Z}\)

Reimplemented from NPbase.

Definition at line 13538 of file NPSMEFTd6.cpp.

13539 {
13540  /* From arXiv:1708.09079 [hep-ph]. In our case, delta_e=0 since it is taken as inputs and its effects propagated
13541  * everywhere else */
13542  double dgEff;
13543 
13544  dgEff = (1.0/ cW2_tree) * ( (cW2_tree - sW2_tree)*deltaGL_f(leptons[ELECTRON])/gZlL +
13547 
13548  return dgEff + deltag1ZNP() ;
13549 }

◆ deltaG2_hWW()

double NPSMEFTd6::deltaG2_hWW ( ) const
virtual

The new physics contribution to the coupling of the effective interaction \(H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}\).

Returns
\(\delta g_{HWW}^{(2)}\)

Reimplemented from NPbase.

Definition at line 2939 of file NPSMEFTd6.cpp.

2940 {
2941  return ( - sqrt( M_PI * aleMz ) * ( CiDHW / sW_tree ) * v2_over_LambdaNP2 / v());
2942 }

◆ deltaG2_hZA()

double NPSMEFTd6::deltaG2_hZA ( ) const
virtual

The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu F^{\mu\nu}\).

Returns
\(\delta g_{HZA}^{(2)}\)

Reimplemented from NPbase.

Definition at line 3057 of file NPSMEFTd6.cpp.

3058 {
3059  return ( sqrt( M_PI * aleMz ) * ( CiDHB / sW_tree - CiDHW / cW_tree ) * v2_over_LambdaNP2 / v());
3060 }

◆ deltaG2_hZZ()

double NPSMEFTd6::deltaG2_hZZ ( ) const
virtual

The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu Z^{\mu\nu}\).

Returns
\(\delta g_{HZZ}^{(2)}\)

Reimplemented from NPbase.

Definition at line 2960 of file NPSMEFTd6.cpp.

2961 {
2962  return ( - sqrt( M_PI * aleMz ) * ( CiDHB / cW_tree + CiDHW / sW_tree ) * v2_over_LambdaNP2 / v());
2963 }

◆ deltaG3_hWW()

double NPSMEFTd6::deltaG3_hWW ( ) const
virtual

The new physics contribution to the coupling of the effective interaction \(H W_{\mu}^\dagger W^{\mu}\).

Returns
\(\delta g_{HWW}^{(3)}\)

Reimplemented from NPbase.

Definition at line 2944 of file NPSMEFTd6.cpp.

2945 {
2946  double NPindirect;
2947 
2948  NPindirect = 2.0 * cW2_tree * Mz * Mz / v()
2949  * (delta_h - 1.0 / 2.0 / (cW2_tree - sW2_tree)
2950  * ((4.0 * sW_tree * cW_tree * CiHWB + cW2_tree * CiHD) * v2_over_LambdaNP2 + DeltaGF()));
2951 
2952  return NPindirect;
2953 }

◆ deltaG3_hZZ()

double NPSMEFTd6::deltaG3_hZZ ( ) const
virtual

The new physics contribution to the coupling of the effective interaction \(H Z_{\mu} Z^{\mu}\).

Returns
\(\delta g_{HZZ}^{(3)}\)

Reimplemented from NPbase.

Definition at line 2965 of file NPSMEFTd6.cpp.

2966 {
2967  double NPindirect = Mz * Mz / v() * (-0.5 * CiHD * v2_over_LambdaNP2 + delta_h - 0.5 * DeltaGF());
2968  double NPdirect = Mz * Mz / v() * CiHD * v2_over_LambdaNP2;
2969  return (NPindirect + NPdirect);
2970 }

◆ deltag3G()

double NPSMEFTd6::deltag3G ( ) const

The new physics contribution to the coupling of the effective interaction \(f_{ABC} G_{\mu\nu}^A G_{\nu\rho}^B G_{\rho\mu}^C\).

Returns
\(\delta g_{3G}\)

Definition at line 3217 of file NPSMEFTd6.cpp.

3218 {
3219  /* Set to 0. for the moment */
3220 
3221  return 0.;
3222 }

◆ deltaG_Aff()

gslpp::complex NPSMEFTd6::deltaG_Aff ( const Particle  p) const

The new physics contribution to the coupling of the effective interaction \(A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).

Parameters
[in]pa lepton or quark
Returns
\(\delta g_{Aff}\)

Definition at line 3210 of file NPSMEFTd6.cpp.

3211 {
3212  /* Set to 0. for the moment */
3213 
3214  return 0.;
3215 }

◆ deltaG_Gff()

gslpp::complex NPSMEFTd6::deltaG_Gff ( const Particle  p) const

The new physics contribution to the coupling of the effective interaction \(G_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).

Parameters
[in]pa lepton or quark
Returns
\(\delta g_{Gff}\)

Definition at line 3196 of file NPSMEFTd6.cpp.

3197 {
3198  /* Set to 0. for the moment */
3199 
3200  return 0.;
3201 }

◆ deltaG_hAA()

double NPSMEFTd6::deltaG_hAA ( ) const
virtual

The new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\).

Returns
\(\delta g_{HAA}\)

Reimplemented from NPbase.

Definition at line 3062 of file NPSMEFTd6.cpp.

3063 {
3064  return (delta_AA / v());
3065 }

◆ deltaG_hAARatio()

double NPSMEFTd6::deltaG_hAARatio ( ) const
virtual

The full new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.

Returns
\(\delta g_{HAA}/g_{HAA}^SM}\)

Reimplemented from NPbase.

Definition at line 3067 of file NPSMEFTd6.cpp.

3068 {
3069  double m_t = mtpole;
3070  double m_b = quarks[BOTTOM].getMass();
3071  double m_c = quarks[CHARM].getMass();
3072  double m_tau = leptons[TAU].getMass();
3073  double m_mu = leptons[MU].getMass();
3074 
3075  double M_w_2 = (trueSM.Mw())*(trueSM.Mw());
3076 
3077  double Qt = quarks[TOP].getCharge();
3078  double Qb = quarks[BOTTOM].getCharge();
3079  double Qc = quarks[CHARM].getCharge();
3080  double Qtau = leptons[TAU].getCharge();
3081  double Qmu = leptons[MU].getCharge();
3082 
3083  double tau_t = 4.0 * m_t * m_t / mHl / mHl;
3084  double tau_b = 4.0 * m_b * m_b / mHl / mHl;
3085  double tau_c = 4.0 * m_c * m_c / mHl / mHl;
3086  double tau_tau = 4.0 * m_tau * m_tau / mHl / mHl;
3087  double tau_mu = 4.0 * m_mu * m_mu / mHl / mHl;
3088  double tau_W = 4.0 * M_w_2 / mHl / mHl;
3089 
3090  double aPiv = ale / 8.0 / M_PI / v();
3091  gslpp::complex gSM, dg;
3092  gslpp::complex dKappa_t = cLHd6 * deltaG_hff(quarks[TOP]) / (-m_t / v());
3093  gslpp::complex dKappa_b = cLHd6 * deltaG_hff(quarks[BOTTOM]) / (-m_b / v());
3094  gslpp::complex dKappa_c = cLHd6 * deltaG_hff(quarks[CHARM]) / (-m_c / v());
3095  gslpp::complex dKappa_tau = cLHd6 * deltaG_hff(leptons[TAU]) / (-m_tau / v());
3096  gslpp::complex dKappa_mu = cLHd6 * deltaG_hff(leptons[MU]) / (-m_mu / v());
3097  double dKappa_W = cLHd6 * (0.5 * v() / M_w_2)*deltaG3_hWW();
3098 
3099  double deltaloc = deltaG_hAA();
3100 
3101  gSM = aPiv * (3.0*Qt*Qt*AH_f(tau_t) +
3102  3.0*Qb*Qb*AH_f(tau_b) +
3103  3.0*Qc*Qc*AH_f(tau_c) +
3104  Qtau*Qtau*AH_f(tau_tau) +
3105  Qmu*Qmu*AH_f(tau_mu) +
3106  AH_W(tau_W));
3107 
3108  dg = deltaloc/gSM + (aPiv/gSM) * (
3109  3.0*Qt*Qt*dKappa_t*AH_f(tau_t) +
3110  3.0*Qb*Qb*dKappa_b*AH_f(tau_b) +
3111  3.0*Qc*Qc*dKappa_c*AH_f(tau_c) +
3112  dKappa_tau*Qtau*Qtau*AH_f(tau_tau) +
3113  dKappa_mu*Qmu*Qmu*AH_f(tau_mu) +
3114  dKappa_W*AH_W(tau_W)
3115  );
3116 
3117  return dg.real();
3118 }

◆ deltaG_hAff()

gslpp::complex NPSMEFTd6::deltaG_hAff ( const Particle  p) const

The new physics contribution to the coupling of the effective interaction \(H A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).

Parameters
[in]pa lepton or quark
Returns
\(\delta g_{hAff}\)

Definition at line 3189 of file NPSMEFTd6.cpp.

3190 {
3191  /* Set to 0. for the moment */
3192 
3193  return 0.;
3194 }

◆ deltaG_hff()

gslpp::complex NPSMEFTd6::deltaG_hff ( const Particle  p) const
virtual

The new physics contribution to the coupling of the effective interaction \(H f\bar{f}\).

Parameters
[in]pa lepton or quark
Returns
\(\delta g_{Hff}\)

Reimplemented from NPbase.

Definition at line 3120 of file NPSMEFTd6.cpp.

3121 {
3122  /* The effects of the RG running are neglected. */
3123  double mf;
3124  if (p.is("TOP"))
3125  //mf = p.getMass(); // m_t(m_t)
3126  mf = mtpole; // pole mass
3127  else
3128  mf = p.getMass();
3129  gslpp::complex CfH = CfH_diag(p);
3130  return (-mf / v() * (delta_h - 0.5 * DeltaGF())
3131  + CfH * v2_over_LambdaNP2 / sqrt(2.0));
3132 }

◆ deltaG_hGff()

gslpp::complex NPSMEFTd6::deltaG_hGff ( const Particle  p) const

The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).

Parameters
[in]pa lepton or quark
Returns
\(\delta g_{hGff}\)

Definition at line 3175 of file NPSMEFTd6.cpp.

3176 {
3177  /* Set to 0. for the moment */
3178 
3179  return 0.;
3180 }

◆ deltaG_hgg()

double NPSMEFTd6::deltaG_hgg ( ) const
virtual

The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\).

Returns
\(\delta g_{HGG}\)

Reimplemented from NPbase.

Definition at line 2907 of file NPSMEFTd6.cpp.

2908 {
2909  return (CHG * v2_over_LambdaNP2 / v());
2910 }

◆ deltaG_hggRatio()

double NPSMEFTd6::deltaG_hggRatio ( ) const
virtual

The full new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.

Returns
\(\delta g_{HGG}/g_{HGG}^SM}\)

Reimplemented from NPbase.

Definition at line 2912 of file NPSMEFTd6.cpp.

2913 {
2914  double m_t = mtpole;
2915  double m_b = quarks[BOTTOM].getMass();
2916  double m_c = quarks[CHARM].getMass();
2917  double tau_t = 4.0 * m_t * m_t / mHl / mHl;
2918  double tau_b = 4.0 * m_b * m_b / mHl / mHl;
2919  double tau_c = 4.0 * m_c * m_c / mHl / mHl;
2920  double aSPiv = AlsMz / 16.0 / M_PI / v();
2921  gslpp::complex gSM, dg;
2922  gslpp::complex dKappa_t = cLHd6 * deltaG_hff(quarks[TOP]) / (-m_t / v());
2923  gslpp::complex dKappa_b = cLHd6 * deltaG_hff(quarks[BOTTOM]) / (-m_b / v());
2924  gslpp::complex dKappa_c = cLHd6 * deltaG_hff(quarks[CHARM]) / (-m_c / v());
2925  double deltaloc = deltaG_hgg();
2926 
2927  gSM = aSPiv * (AH_f(tau_t) + AH_f(tau_b) + AH_f(tau_c));
2928 
2929  dg = deltaloc/gSM + (aSPiv/gSM) * (dKappa_t*AH_f(tau_t) + dKappa_b*AH_f(tau_b) + dKappa_c*AH_f(tau_c));
2930 
2931  return dg.real();
2932 }

◆ deltaG_hhhRatio()

double NPSMEFTd6::deltaG_hhhRatio ( ) const
virtual

The new physics contribution to the Higgs self-coupling \( H H H\). Normalized to the SM value.

Returns
\(\delta g_{HHH}/g_{HHH}^SM}\)

Reimplemented from NPbase.

Definition at line 3134 of file NPSMEFTd6.cpp.

3135 {
3136  double dg;
3137 
3138  dg = -0.5 * DeltaGF() + 3.0 * delta_h - 2.0 * CiH * v2_over_LambdaNP2 * v2/mHl/mHl;
3139 
3140  return dg;
3141 }

◆ deltaG_hZff()

gslpp::complex NPSMEFTd6::deltaG_hZff ( const Particle  p) const

The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).

Parameters
[in]pa lepton or quark
Returns
\(\delta g_{hZff}\)

Definition at line 3182 of file NPSMEFTd6.cpp.

3183 {
3184  /* Set to 0. for the moment */
3185 
3186  return 0.;
3187 }

◆ deltaG_Zff()

gslpp::complex NPSMEFTd6::deltaG_Zff ( const Particle  p) const

The new physics contribution to the coupling of the effective interaction \(Z_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).

Parameters
[in]pa lepton or quark
Returns
\(\delta g_{Zff}\)

Definition at line 3203 of file NPSMEFTd6.cpp.

3204 {
3205  /* Set to 0. for the moment */
3206 
3207  return 0.;
3208 }

◆ deltaGA_f()

double NPSMEFTd6::deltaGA_f ( const Particle  p) const
virtual

New physics contribution to the neutral-current axial-vector coupling \(g_A^f\).

Parameters
[in]fa lepton or quark
Returns
\(\delta g_A^f\)

Reimplemented from NPbase.

Definition at line 2847 of file NPSMEFTd6.cpp.

2848 {
2849  return (deltaGL_f(p) - deltaGR_f(p));
2850 }

◆ deltaGamma_W()

double NPSMEFTd6::deltaGamma_W ( ) const
virtual

The new physics contribution to the total decay width of the \(W\) boson, \(\delta \Gamma_W\).

Returns
\(\delta \Gamma_W\) in GeV

Reimplemented from NPbase.

Definition at line 2800 of file NPSMEFTd6.cpp.

2801 {
2802  double G0 = GF * pow(Mz*cW_tree, 3.0) / 6.0 / sqrt(2.0) / M_PI;
2803  double GammaW_tree = (3.0 + 2.0 * Nc) * G0;
2804 
2805  return (- 3.0 * GammaW_tree / 4.0 / (cW2_tree - sW2_tree)
2806  *(4.0 * sW_tree * cW_tree * CiHWB * v2_over_LambdaNP2
2808  + 2.0 * (1.0 + cW2_tree) / 3.0 * DeltaGF())
2809  + 2.0 * G0 * (CiHL3_11 + CiHL3_22 + CiHL3_33 + Nc*(CiHQ3_11 + CiHQ3_22)) * v2_over_LambdaNP2);
2810 // + 2.0 * GammaW_tree / 3.0 * (CiHL3_11 + CiHQ3_11 + CiHQ3_22) * v2_over_LambdaNP2);
2811 }

◆ deltaGamma_Wff()

double NPSMEFTd6::deltaGamma_Wff ( const Particle  fi,
const Particle  fj 
) const
virtual

The new physics contribution to the decay width of the \(W\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\).

Parameters
[in]fia lepton or quark
[in]fja lepton or quark
Returns
\(\delta \Gamma_W^{ff}\) in GeV

Reimplemented from NPbase.

Definition at line 2766 of file NPSMEFTd6.cpp.

2767 {
2768  double G0 = GF * pow(Mz*cW_tree, 3.0) / 6.0 / sqrt(2.0) / M_PI;
2769  double deltaGamma_Wij;
2770  double GammaW_tree;
2771  double CHF3ij;
2772 
2773  if (fj.getIndex() - fi.getIndex() == 1)
2774  CHF3ij = CHF3_diag(fi);
2775  else
2776  CHF3ij = 0.;
2777 
2778  if (fi.is("QUARK")) {
2779  GammaW_tree = Nc * G0;
2780  } else {
2781  GammaW_tree = G0;
2782  }
2783 
2784  deltaGamma_Wij = - 3.0 * GammaW_tree / 4.0 / (cW2_tree - sW2_tree)
2785  *(4.0 * sW_tree * cW_tree * CiHWB * v2_over_LambdaNP2
2787  + 2.0 * (1.0 + cW2_tree) / 3.0 * DeltaGF());
2788 
2789  deltaGamma_Wij = deltaGamma_Wij + 2.0 * GammaW_tree * CHF3ij * v2_over_LambdaNP2;
2790 
2791  return deltaGamma_Wij;
2792 }

◆ deltaGammaHbbRatio1()

double NPSMEFTd6::deltaGammaHbbRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to bb)\)/ \(\Gamma(H\to bb)_{\mathrm{SM}}\)

Definition at line 12339 of file NPSMEFTd6.cpp.

12340 {
12341  double dwidth = 0.0;
12342 
12343  double C1 = 0.0;
12344 
12345  if (FlagLoopHd6) {
12346 
12347  dwidth = ( +121248. * CiHbox / LambdaNP2
12348  -558.186 * CiuH_33r / LambdaNP2
12349  -5027051. * CidH_33r / LambdaNP2
12350  -30312.1 * CiHD / LambdaNP2
12351  -60624.1 * DeltaGF() / v() / v() );
12352 
12353  } else {
12354 
12355  dwidth = ( +121248. * CiHbox / LambdaNP2
12356  -5050180. * CidH_33r / LambdaNP2
12357  -30312.1 * CiHD / LambdaNP2
12358  -60624.1 * DeltaGF() / v() / v() );
12359  }
12360 
12361 // Linear contribution from Higgs self-coupling
12362  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
12363 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
12364  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
12365 
12366  // Add modifications due to small variations of the SM parameters
12367  dwidth += cHSM * ( +1. * deltaGmu()
12368  -0.23 * deltaaSMZ()
12369  +1.007 * deltaMh()
12370  +0.001 * deltamt()
12371  +1.992 * deltamb() );
12372 
12373  // SM (1) + intrinsic + parametric theory relative errors (free pars)
12374  dwidth += eHbbint + eHbbpar;
12375 
12376  return dwidth;
12377 }

◆ deltaGammaHbbRatio2()

double NPSMEFTd6::deltaGammaHbbRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to bb)\)/ \(\Gamma(H\to bb)_{\mathrm{SM}}\)

Definition at line 12379 of file NPSMEFTd6.cpp.

12380 {
12381  double dwidth = 0.0;
12382 
12383 
12384  //Contributions that are quadratic in the effective coefficients
12385  return ( dwidth );
12386 
12387 }

◆ deltaGammaHccRatio1()

double NPSMEFTd6::deltaGammaHccRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to cc)\)/ \(\Gamma(H\to cc)_{\mathrm{SM}}\)

Definition at line 12274 of file NPSMEFTd6.cpp.

12275 {
12276  double dwidth = 0.0;
12277 
12278  double C1 = 0.0;
12279 
12280  if (FlagLoopHd6) {
12281 
12282  dwidth = ( +121248. * CiHbox / LambdaNP2
12283  -16421890. * CiuH_22r / LambdaNP2
12284  -992.159 * CiuH_33r / LambdaNP2
12285  -30312.1 * CiHD / LambdaNP2
12286  -60624.1 * DeltaGF() / v() / v() );
12287 
12288  } else {
12289 
12290  dwidth = ( +121248. * CiHbox / LambdaNP2
12291  -16556668. * CiuH_22r / LambdaNP2
12292  -30312.1 * CiHD / LambdaNP2
12293  -60624.1 * DeltaGF() / v() / v() );
12294  }
12295 
12296 // Linear contribution from Higgs self-coupling
12297  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
12298 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
12299  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
12300 
12301  // Add modifications due to small variations of the SM parameters
12302  dwidth += cHSM * ( +1. * deltaGmu()
12303  -0.789 * deltaaSMZ()
12304  +1.004 * deltaMh()
12305  +0.001 * deltamt()
12306  +1.995 * deltamc() );
12307 
12308  // SM (1) + intrinsic + parametric theory relative errors (free pars)
12309  dwidth += eHccint + eHccpar;
12310 
12311  return dwidth;
12312 }

◆ deltaGammaHccRatio2()

double NPSMEFTd6::deltaGammaHccRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to cc)\)/ \(\Gamma(H\to cc)_{\mathrm{SM}}\)

Definition at line 12314 of file NPSMEFTd6.cpp.

12315 {
12316  double dwidth = 0.0;
12317 
12318 
12319  //Contributions that are quadratic in the effective coefficients
12320  return ( dwidth );
12321 
12322 }

◆ deltaGammaHgagaRatio1()

double NPSMEFTd6::deltaGammaHgagaRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to \gamma\gamma)\)/ \(\Gamma(H\to \gamma\gamma)_{\mathrm{SM}}\)

Definition at line 12093 of file NPSMEFTd6.cpp.

12094 {
12095  double dwidth = 0.0;
12096 
12097  double C1 = 0.0049;
12098 
12099 // It does not include modifications of MW
12100 
12101 // Write the tree-level contributions directly as a function
12102 // of delta_AA (or deltaG_hAA) to account for variations of sw2 and cw2
12103 
12104  dwidth = ( -255156.97*deltaG_hAA()
12105 // -48314158. * CiHB / LambdaNP2
12106 // -14510502. * CiHW / LambdaNP2
12107 // +26477588. * CiHWB / LambdaNP2
12108  + cLHd6 * (
12109  +119766. * CiHbox / LambdaNP2
12110  -42565.7 * CieH_33r / LambdaNP2
12111  -48868.1 * CiuH_22r / LambdaNP2
12112  +32078.2 * CiuH_33r / LambdaNP2
12113  -18428.3 * CidH_33r / LambdaNP2
12114  -137452. * CiHD / LambdaNP2
12115  -235677. * CiHWB / LambdaNP2
12116  -124462. * DeltaGF() / v() / v()
12117  -1.257 * deltaMwd6() )
12118  );
12119 
12120 // Linear contribution from Higgs self-coupling
12121  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
12122 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
12123  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
12124 
12125  // Add modifications due to small variations of the SM parameters
12126  dwidth += cHSM * ( +2. * deltaa0()
12127  +0.27 * deltaaMZ()
12128  +0.736 * deltaGmu()
12129  -1.797 * deltaMz()
12130  +0.02 * deltaaSMZ()
12131  +4.195 * deltaMh()
12132  +0.047 * deltamt()
12133  +0.008 * deltamb()
12134  +0.009 * deltamc()
12135  +0.01 * deltamtau() );
12136 
12137  // SM (1) + intrinsic + parametric theory relative errors (free pars)
12138  dwidth += eHgagaint + eHgagapar;
12139 
12140  return dwidth;
12141 }

◆ deltaGammaHgagaRatio2()

double NPSMEFTd6::deltaGammaHgagaRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to \gamma\gamma)\)/ \(\Gamma(H\to \gamma\gamma)_{\mathrm{SM}}\)

Definition at line 12143 of file NPSMEFTd6.cpp.

12144 {
12145  double dwidth = 0.0;
12146 
12147 
12148  //Contributions that are quadratic in the effective coefficients
12149  return ( dwidth );
12150 
12151 }

◆ deltaGammaHggRatio1()

double NPSMEFTd6::deltaGammaHggRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients.

Returns
\(\delta \Gamma(H\to gg)\)/ \(\Gamma(H\to gg)_{\mathrm{SM}}\)

Definition at line 10664 of file NPSMEFTd6.cpp.

10665 {
10666  double dwidth = 0.0;
10667 
10668  double C1 = 0.0066;
10669 
10670  dwidth = ( +37526258. * CHG / LambdaNP2
10671  + cLHd6 * (
10672  +121248. * CiHbox / LambdaNP2
10673  +173353. * CiuH_22r / LambdaNP2
10674  -129155. * CiuH_33r / LambdaNP2
10675  +248530. * CidH_33r / LambdaNP2
10676  -30312.1 * CiHD / LambdaNP2
10677  -60624.1 * DeltaGF() / v() / v() )
10678  );
10679 
10680 // Linear contribution from Higgs self-coupling
10681  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
10682 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
10683  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
10684 
10685  // Add modifications due to small variations of the SM parameters
10686  dwidth += cHSM * ( +1.003 * deltaGmu()
10687  +2.31 * deltaaSMZ()
10688  +3.276 * deltaMh()
10689  -0.134 * deltamt()
10690  -0.106 * deltamb()
10691  -0.03 * deltamc() );
10692 
10693  // SM (1) + intrinsic + parametric theory relative errors (free pars)
10694  dwidth += eHggint + eHggpar;
10695 
10696  return dwidth;
10697 }

◆ deltaGammaHggRatio2()

double NPSMEFTd6::deltaGammaHggRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to gg)\)/ \(\Gamma(H\to gg)_{\mathrm{SM}}\)

Definition at line 10699 of file NPSMEFTd6.cpp.

10700 {
10701  double dwidth = 0.0;
10702 
10703 
10704  //Contributions that are quadratic in the effective coefficients
10705  return ( dwidth );
10706 
10707 }

◆ deltaGammaHmumuRatio1()

double NPSMEFTd6::deltaGammaHmumuRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to \mu\mu)\)/ \(\Gamma(H\to \mu\mu)_{\mathrm{SM}}\)

Definition at line 12169 of file NPSMEFTd6.cpp.

12170 {
12171  double dwidth = 0.0;
12172 
12173  double C1 = 0.0;
12174 
12175  dwidth = ( +121248. * CiHbox / LambdaNP2
12176  -199792511. * CieH_22r / LambdaNP2
12177  -30312.1 * CiHD / LambdaNP2
12178  -60624.1 * DeltaGF() / v() / v() );
12179 
12180 // Linear contribution from Higgs self-coupling
12181  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
12182 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
12183  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
12184 
12185  // Add modifications due to small variations of the SM parameters
12186  dwidth += cHSM * ( +1. * deltaGmu()
12187  +1. * deltaMh() );
12188 
12189  // SM (1) + intrinsic + parametric theory relative errors (free pars)
12190  dwidth += eHmumuint + eHmumupar;
12191 
12192  return dwidth;
12193 }

◆ deltaGammaHmumuRatio2()

double NPSMEFTd6::deltaGammaHmumuRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to \mu\mu)\)/ \(\Gamma(H\to \mu\mu)_{\mathrm{SM}}\)

Definition at line 12195 of file NPSMEFTd6.cpp.

12196 {
12197  double dwidth = 0.0;
12198 
12199 
12200  //Contributions that are quadratic in the effective coefficients
12201  return ( dwidth );
12202 
12203 }

◆ deltaGammaHtautauRatio1()

double NPSMEFTd6::deltaGammaHtautauRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to \tau\tau)\)/ \(\Gamma(H\to \tau\tau)_{\mathrm{SM}}\)

Definition at line 12221 of file NPSMEFTd6.cpp.

12222 {
12223  double dwidth = 0.0;
12224 
12225  double C1 = 0.0;
12226 
12227  dwidth = ( +121248. * CiHbox / LambdaNP2
12228  -11880369. * CieH_33r / LambdaNP2
12229  -30312.1 * CiHD / LambdaNP2
12230  -60624.1 * DeltaGF() / v() / v() );
12231 
12232 // Linear contribution from Higgs self-coupling
12233  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
12234 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
12235  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
12236 
12237  // Add modifications due to small variations of the SM parameters
12238  dwidth += cHSM * ( +1. * deltaGmu()
12239  +1.002 * deltaMh()
12240  +1.998 * deltamtau() );
12241 
12242  // SM (1) + intrinsic + parametric theory relative errors (free pars)
12243  dwidth += eHtautauint + eHtautaupar;
12244 
12245  return dwidth;
12246 }

◆ deltaGammaHtautauRatio2()

double NPSMEFTd6::deltaGammaHtautauRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to \tau\tau)\)/ \(\Gamma(H\to \tau\tau)_{\mathrm{SM}}\)

Definition at line 12248 of file NPSMEFTd6.cpp.

12249 {
12250  double dwidth = 0.0;
12251 
12252 
12253  //Contributions that are quadratic in the effective coefficients
12254  return ( dwidth );
12255 
12256 }

◆ deltaGammaHWffRatio1()

double NPSMEFTd6::deltaGammaHWffRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to W f f)\)/ \(\Gamma(H\to W f f)_{\mathrm{SM}}\)

Definition at line 11006 of file NPSMEFTd6.cpp.

11007 {
11008  double dwidth = 0.0;
11009 
11010  double C1 = 0.0073;
11011 
11012  dwidth = ( +121288. * CiHbox / LambdaNP2
11013  +5395.21 * (1.0/3.0) * ( CiHL3_11 + CiHL3_22 + CiHL3_33 ) / LambdaNP2
11014  +11680.9 * (1.0/2.0) * ( CiHQ3_11 + CiHQ3_22 ) / LambdaNP2
11015  -159787. * CiHD / LambdaNP2
11016  -91509.1 * CiHW / LambdaNP2
11017  -283092. * CiHWB / LambdaNP2
11018  +37845.1 * CiDHW / LambdaNP2
11019  -3.259 * DeltaGF()
11020  -15.196 * deltaMwd6() );
11021 
11022 // Linear contribution from Higgs self-coupling
11023  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11024 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11025  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11026 
11027  // Add modifications due to small variations of the SM parameters
11028  //dwidth += cHSM * ( 0.0 );
11029 
11030  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11031  //dwidth += eHWWint + eHWWpar;
11032 
11033  return dwidth;
11034 
11035 }

◆ deltaGammaHWffRatio2()

double NPSMEFTd6::deltaGammaHWffRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to W f f)\)/ \(\Gamma(H\to W f f)_{\mathrm{SM}}\)

Definition at line 11037 of file NPSMEFTd6.cpp.

11038 {
11039  double dwidth = 0.0;
11040 
11041 
11042  //Contributions that are quadratic in the effective coefficients
11043  return ( dwidth );
11044 
11045 }

◆ deltaGammaHWjjRatio1()

double NPSMEFTd6::deltaGammaHWjjRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to W j j)\)/ \(\Gamma(H\to W j j)_{\mathrm{SM}}\)

Definition at line 10890 of file NPSMEFTd6.cpp.

10891 {
10892  double dwidth = 0.0;
10893 
10894  double C1 = 0.0073;
10895 
10896  dwidth = ( +121611. * CiHbox / LambdaNP2
10897  +17701.4 * (1.0/2.0) * ( CiHQ3_11 + CiHQ3_22 ) / LambdaNP2
10898  -159273. * CiHD / LambdaNP2
10899  -91021.6 * CiHW / LambdaNP2
10900  -282574. * CiHWB / LambdaNP2
10901  +37917.5 * CiDHW / LambdaNP2
10902  -3.259 * DeltaGF()
10903  -15.198 * deltaMwd6() );
10904 
10905 // Linear contribution from Higgs self-coupling
10906  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
10907 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
10908  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
10909 
10910  // Add modifications due to small variations of the SM parameters
10911  //dwidth += cHSM * ( 0.0 );
10912 
10913  // SM (1) + intrinsic + parametric theory relative errors (free pars)
10914  //dwidth += eHWWint + eHWWpar;
10915 
10916  return dwidth;
10917 
10918 }

◆ deltaGammaHWjjRatio2()

double NPSMEFTd6::deltaGammaHWjjRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to W j j)\)/ \(\Gamma(H\to W j j)_{\mathrm{SM}}\)

Definition at line 10920 of file NPSMEFTd6.cpp.

10921 {
10922  double dwidth = 0.0;
10923 
10924 
10925  //Contributions that are quadratic in the effective coefficients
10926  return ( dwidth );
10927 
10928 }

◆ deltaGammaHWlvRatio1()

double NPSMEFTd6::deltaGammaHWlvRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Wl\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Wl\nu)\)/ \(\Gamma(H\to Wl\nu)_{\mathrm{SM}}\)

Definition at line 10773 of file NPSMEFTd6.cpp.

10774 {
10775  double dwidth = 0.0;
10776 
10777  double C1 = 0.0073;
10778 
10779  dwidth = ( +121875. * CiHbox / LambdaNP2
10780  +18351.9 * (1.0/2.0) * ( CiHL3_11 + CiHL3_22 ) / LambdaNP2
10781  -159873. * CiHD / LambdaNP2
10782  -91288.7 * CiHW / LambdaNP2
10783  -284689. * CiHWB / LambdaNP2
10784  +37703.7 * CiDHW / LambdaNP2
10785  -3.292 * DeltaGF()
10786  -15.14 * deltaMwd6() );
10787 
10788 // Linear contribution from Higgs self-coupling
10789  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
10790 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
10791  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
10792 
10793  // Add modifications due to small variations of the SM parameters
10794  //dwidth += cHSM * ( 0.0 );
10795 
10796  // SM (1) + intrinsic + parametric theory relative errors (free pars)
10797  //dwidth += eHWWint + eHWWpar;
10798 
10799  return dwidth;
10800 
10801 }

◆ deltaGammaHWlvRatio2()

double NPSMEFTd6::deltaGammaHWlvRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Wl\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Wl\nu)\)/ \(\Gamma(H\to Wl\nu)_{\mathrm{SM}}\)

Definition at line 10803 of file NPSMEFTd6.cpp.

10804 {
10805  double dwidth = 0.0;
10806 
10807 
10808  //Contributions that are quadratic in the effective coefficients
10809  return ( dwidth );
10810 
10811 }

◆ deltaGammaHWW2l2vRatio1()

double NPSMEFTd6::deltaGammaHWW2l2vRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to WW^*\to l\nu l\nu)\)/ \(\Gamma(H\to WW^*\to l\nu l\nu)_{\mathrm{SM}}\)

Definition at line 10829 of file NPSMEFTd6.cpp.

10830 {
10831  double dwidth = 0.0;
10832 
10833  double C1 = 0.0073;
10834 
10835  dwidth = ( +120742. * CiHbox / LambdaNP2
10836  +131582. * (1.0/2.0) * ( CiHL3_11 + CiHL3_22 ) / LambdaNP2
10837  -204043. * CiHD / LambdaNP2
10838  -91463.9 * CiHW / LambdaNP2
10839  -379529. * CiHWB / LambdaNP2
10840  +36848.2 * CiDHW / LambdaNP2
10841  -4.705 * DeltaGF()
10842  -13.735 * deltaMwd6()
10843  -0.965 * deltaGwd6()
10844  );
10845 
10846 // Linear contribution from Higgs self-coupling
10847  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
10848 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
10849  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
10850 
10851  // Add modifications due to small variations of the SM parameters
10852  dwidth += cHSM * ( -12.123 * deltaMz()
10853  +13.615 * deltaMh()
10854  +1.756 * deltaaMZ()
10855  +0.216 * deltaGmu() );
10856 
10857  // SM (1) + intrinsic + parametric theory relative errors (free pars)
10858  dwidth += eHWWint + eHWWpar;
10859 
10860  return dwidth;
10861 
10862 }

◆ deltaGammaHWW2l2vRatio2()

double NPSMEFTd6::deltaGammaHWW2l2vRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to WW^*\to l\nu l\nu)\)/ \(\Gamma(H\to WW^*\to l\nu l\nu)_{\mathrm{SM}}\)

Definition at line 10864 of file NPSMEFTd6.cpp.

10865 {
10866  double dwidth = 0.0;
10867 
10868 
10869  //Contributions that are quadratic in the effective coefficients
10870  return ( dwidth );
10871 
10872 }

◆ deltaGammaHWW4fRatio1()

double NPSMEFTd6::deltaGammaHWW4fRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to WW^*\to 4f)\)/ \(\Gamma(H\to WW^*\to 4f)_{\mathrm{SM}}\)

Definition at line 11063 of file NPSMEFTd6.cpp.

11064 {
11065  double dwidth = 0.0;
11066 
11067  double C1 = 0.0073;
11068 
11069  double CWff, sf;
11070 
11071  CWff = ( CiHL3_11 + CiHL3_22 + CiHL3_33 ) * v2_over_LambdaNP2 +
11073 
11074  CWff = CWff/( 3.0 + 2.0*Nc );
11075 
11076  sf = 90362.5 * (1.0/2.0) * ( 3.0 + 2.0*Nc )/(Nc*v2) ; // Coefficient of the CWff term. From the CiHQ3_11 term in the ME.
11077 
11078  dwidth = ( +121886. * CiHbox / LambdaNP2
11079  + sf* CWff
11080  -204009. * CiHD / LambdaNP2
11081  -91455.7 * CiHW / LambdaNP2
11082  -382903. * CiHWB / LambdaNP2
11083  +38314.9 * CiDHW / LambdaNP2
11084  -4.757 * DeltaGF()
11085  -13.716 * deltaMwd6()
11086  -0.963 * deltaGwd6()
11087  );
11088 
11089 // Linear contribution from Higgs self-coupling
11090  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11091 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11092  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11093 
11094  // Add modifications due to small variations of the SM parameters
11095  dwidth += cHSM * ( -12.271 * deltaMz()
11096  +13.665 * deltaMh()
11097  +1.85 * deltaaMZ()
11098  +0.224 * deltaGmu() );
11099 
11100  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11101  dwidth += eHWWint + eHWWpar;
11102 
11103  return dwidth;
11104 
11105 }

◆ deltaGammaHWW4fRatio2()

double NPSMEFTd6::deltaGammaHWW4fRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to WW^*\to 4f)\)/ \(\Gamma(H\to WW^*\to 4f)_{\mathrm{SM}}\)

Definition at line 11107 of file NPSMEFTd6.cpp.

11108 {
11109  double dwidth = 0.0;
11110 
11111 
11112  //Contributions that are quadratic in the effective coefficients
11113  return ( dwidth );
11114 
11115 }

◆ deltaGammaHWW4jRatio1()

double NPSMEFTd6::deltaGammaHWW4jRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to WW^*\to 4j)\)/ \(\Gamma(H\to WW^*\to 4j)_{\mathrm{SM}}\)

Definition at line 10946 of file NPSMEFTd6.cpp.

10947 {
10948  double dwidth = 0.0;
10949 
10950  double C1 = 0.0073;
10951 
10952  dwidth = ( +121936. * CiHbox / LambdaNP2
10953  +138860. * (1.0/2.0) * ( CiHQ3_11 + CiHQ3_22 ) / LambdaNP2
10954  -205023. * CiHD / LambdaNP2
10955  -89938.5 * CiHW / LambdaNP2
10956  -383944. * CiHWB / LambdaNP2
10957  +38244.6 * CiDHW / LambdaNP2
10958  -4.816 * DeltaGF()
10959  -13.647 * deltaMwd6()
10960  -0.959 * deltaGwd6() );
10961 
10962 // Linear contribution from Higgs self-coupling
10963  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
10964 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
10965  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
10966 
10967  // Add modifications due to small variations of the SM parameters
10968  dwidth += cHSM * ( -12.168 * deltaMz()
10969  +13.66 * deltaMh()
10970  +1.899 * deltaaMZ()
10971  +0.189 * deltaGmu() );
10972 
10973  // SM (1) + intrinsic + parametric theory relative errors (free pars)
10974  dwidth += eHWWint + eHWWpar;
10975 
10976  return dwidth;
10977 
10978 }

◆ deltaGammaHWW4jRatio2()

double NPSMEFTd6::deltaGammaHWW4jRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to WW^*\to 4j)\)/ \(\Gamma(H\to WW^*\to 4j)_{\mathrm{SM}}\)

Definition at line 10980 of file NPSMEFTd6.cpp.

10981 {
10982  double dwidth = 0.0;
10983 
10984 
10985  //Contributions that are quadratic in the effective coefficients
10986  return ( dwidth );
10987 
10988 }

◆ deltaGammaHWWRatio1()

double NPSMEFTd6::deltaGammaHWWRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to WW)\)/ \(\Gamma(H\to WW)_{\mathrm{SM}}\)

Definition at line 10725 of file NPSMEFTd6.cpp.

10726 {
10727  double dwidth = 0.0;
10728 
10729 // double C1 = 0.0073;
10730 
10731  dwidth = deltaGammaHWW4fRatio1();
10732 
10733 // Linear contribution from Higgs self-coupling
10734 // dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
10735 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
10736 // dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
10737 
10738  // SM (1) + intrinsic + parametric theory relative errors (free pars)
10739 // dwidth += eHWWint + eHWWpar;
10740 
10741  return dwidth;
10742 
10743 }

◆ deltaGammaHWWRatio2()

double NPSMEFTd6::deltaGammaHWWRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to WW)\)/ \(\Gamma(H\to WW)_{\mathrm{SM}}\)

Definition at line 10745 of file NPSMEFTd6.cpp.

10746 {
10747  double dwidth = 0.0;
10748 
10749  //Contributions that are quadratic in the effective coefficients
10750  dwidth = deltaGammaHWW4fRatio2();
10751 
10752 
10753  return dwidth;
10754 
10755 }

◆ deltaGammaHZddRatio1()

double NPSMEFTd6::deltaGammaHZddRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z d d)\)/ \(\Gamma(H\to Z d d)_{\mathrm{SM}}\)

Definition at line 11800 of file NPSMEFTd6.cpp.

11801 {
11802  double dwidth = 0.0;
11803 
11804  double C1 = 0.0083;
11805 
11806  dwidth = ( +121756. * CiHbox / LambdaNP2
11807  +9252.73 * (1.0/3.0) * ( CiHQ1_11 + CiHQ1_22 + CiHQ1_33 ) / LambdaNP2
11808  -1471.03 * (1.0/3.0) * ( CiHd_11 + CiHd_22 + CiHd_33 ) / LambdaNP2
11809  +9252.73 * (1.0/3.0) * ( CiHQ3_11 + CiHQ3_22 + CiHQ3_33 ) / LambdaNP2
11810  -12714.3 * CiHD / LambdaNP2
11811  -13589.3 * CiHB / LambdaNP2
11812  -45689.4 * CiHW / LambdaNP2
11813  -85582.3 * CiHWB / LambdaNP2
11814  +17007.1 * CiDHB / LambdaNP2
11815  +30733.1 * CiDHW / LambdaNP2
11816  -2.427 * DeltaGF() );
11817 
11818 // Linear contribution from Higgs self-coupling
11819  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11820 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11821  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11822 
11823  // Add modifications due to small variations of the SM parameters
11824  //dwidth += cHSM * ( 0.0 );
11825 
11826  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11827  //dwidth += eHZZint + eHZZpar;
11828 
11829  return dwidth;
11830 
11831 }

◆ deltaGammaHZddRatio2()

double NPSMEFTd6::deltaGammaHZddRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z d d)\)/ \(\Gamma(H\to Z d d)_{\mathrm{SM}}\)

Definition at line 11833 of file NPSMEFTd6.cpp.

11834 {
11835  double dwidth = 0.0;
11836 
11837 
11838  //Contributions that are quadratic in the effective coefficients
11839  return ( dwidth );
11840 
11841 }

◆ deltaGammaHZeeRatio1()

double NPSMEFTd6::deltaGammaHZeeRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Zee)\)/ \(\Gamma(H\to Zee)_{\mathrm{SM}}\)

Definition at line 11240 of file NPSMEFTd6.cpp.

11241 {
11242  double dwidth = 0.0;
11243 
11244  double C1 = 0.0083;
11245 
11246 // Derived from the HZll expression for l=e only
11247 
11248  dwidth = ( +121715. * CiHbox / LambdaNP2
11249  +8726.9 * CiHL1_11 / LambdaNP2
11250  -7315.2 * CiHe_11 / LambdaNP2
11251  +8726.9 * CiHL3_11 / LambdaNP2
11252  -5544.15 * CiHD / LambdaNP2
11253  -13560.9 * CiHB / LambdaNP2
11254  -45585.2 * CiHW / LambdaNP2
11255  -53507.9 * CiHWB / LambdaNP2
11256  +16829.2 * CiDHB / LambdaNP2
11257  +30766.6 * CiDHW / LambdaNP2
11258  -2.204 * DeltaGF() );
11259 
11260 // Linear contribution from Higgs self-coupling
11261  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11262 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11263  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11264 
11265  // Add modifications due to small variations of the SM parameters
11266  //dwidth += cHSM * ( 0.0 );
11267 
11268  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11269  //dwidth += eHZZint + eHZZpar;
11270 
11271  return dwidth;
11272 
11273 }

◆ deltaGammaHZeeRatio2()

double NPSMEFTd6::deltaGammaHZeeRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Zee)\)/ \(\Gamma(H\to Zee)_{\mathrm{SM}}\)

Definition at line 11275 of file NPSMEFTd6.cpp.

11276 {
11277  double dwidth = 0.0;
11278 
11279 
11280  //Contributions that are quadratic in the effective coefficients
11281  return ( dwidth );
11282 
11283 }

◆ deltaGammaHZffRatio1()

double NPSMEFTd6::deltaGammaHZffRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z ff)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z f f)\)/ \(\Gamma(H\to Z f f)_{\mathrm{SM}}\)

Definition at line 11859 of file NPSMEFTd6.cpp.

11860 {
11861  double dwidth = 0.0;
11862 
11863  double C1 = 0.0083;
11864 
11865  dwidth = ( +121551. * CiHbox / LambdaNP2
11866  -824.482 * (1.0/3.0) * ( CiHL1_11 + CiHL1_22 + CiHL1_33 ) / LambdaNP2
11867  +1840.54 * (1.0/12.0) * ( 5.0 * CiHQ1_11 + 5.0 * CiHQ1_22 + 2.0 * CiHQ1_33 - CiHQ3_11 - CiHQ3_22 + 2.0 * CiHQ3_33 ) / LambdaNP2
11868  -795.383 * (1.0/3.0) * ( CiHe_11 + CiHe_22 + CiHe_33 ) / LambdaNP2
11869  +1069.4 * (1.0/2.0) * ( CiHu_11 + CiHu_22 ) / LambdaNP2
11870  -579.563 * (1.0/3.0) * ( CiHd_11 + CiHd_22 + CiHd_33 ) / LambdaNP2
11871  +3164.56 * (1.0/3.0) * ( CiHL3_11 + CiHL3_22 + CiHL3_33 ) / LambdaNP2
11872  +6413.99 * (-1.0/12.0) * ( CiHQ1_11 + CiHQ1_22 - 2.0 * CiHQ1_33 - 5.0 * CiHQ3_11 - 5.0 * CiHQ3_22 - 2.0 * CiHQ3_33) / LambdaNP2
11873  -10839.5 * CiHD / LambdaNP2
11874  -14222.3 * CiHB / LambdaNP2
11875  -45455.6 * CiHW / LambdaNP2
11876  -75343.1 * CiHWB / LambdaNP2
11877  +16804.9 * CiDHB / LambdaNP2
11878  +30421. * CiDHW / LambdaNP2
11879  -2.356 * DeltaGF() );
11880 
11881 // Linear contribution from Higgs self-coupling
11882  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11883 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11884  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11885 
11886  // Add modifications due to small variations of the SM parameters
11887  //dwidth += cHSM * ( 0.0 );
11888 
11889  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11890  //dwidth += eHZZint + eHZZpar;
11891 
11892  return dwidth;
11893 
11894 }

◆ deltaGammaHZffRatio2()

double NPSMEFTd6::deltaGammaHZffRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z ff)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z f f)\)/ \(\Gamma(H\to Z f f)_{\mathrm{SM}}\)

Definition at line 11896 of file NPSMEFTd6.cpp.

11897 {
11898  double dwidth = 0.0;
11899 
11900 
11901  //Contributions that are quadratic in the effective coefficients
11902  return ( dwidth );
11903 
11904 }

◆ deltaGammaHZgaRatio1()

double NPSMEFTd6::deltaGammaHZgaRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z\gamma)\)/ \(\Gamma(H\to Z\gamma)_{\mathrm{SM}}\)

Definition at line 12008 of file NPSMEFTd6.cpp.

12009 {
12010  double dwidth = 0.0;
12011 
12012  double C1 = 0.0;
12013 
12014 // It includes modifications of Zff vertices and MW, but not on the pure VVV and VVVV vertices
12015 
12016 // Write the tree-level contributions directly as a function
12017 // of delta_ZA (or deltaG1_hZA()) to account for variations of sw2 and cw2
12018 
12019  dwidth = ( -71769.02 * deltaG1_hZA()
12020 // +14894914. * CiHB / LambdaNP2
12021 // -14894913. * CiHW / LambdaNP2
12022 // +9508089. * CiHWB / LambdaNP2
12023 // -2869576. * CiDHB / LambdaNP2
12024 // +1572613. * CiDHW / LambdaNP2
12025  + cLHd6 * (
12026  +120002. * CiHbox / LambdaNP2
12027  +50.12 * CiHL1_33 / LambdaNP2
12028  +17401. * CiHQ1_33 / LambdaNP2
12029  +50.12 * CiHe_33 / LambdaNP2
12030  +17188.7 * CiHu_33 / LambdaNP2
12031  +212.376 * CiHd_33 / LambdaNP2
12032  +50.12 * CiHL3_33 / LambdaNP2
12033  -16976.3 * CiHQ3_33 / LambdaNP2
12034  -373.856 * CieH_33r / LambdaNP2
12035  -2953.05 * CiuH_22r / LambdaNP2
12036  +6636.34 * CiuH_33r / LambdaNP2
12037  -6121.66 * CidH_33r / LambdaNP2
12038  -111254. * CiHD / LambdaNP2
12039  -162538. * CiHWB / LambdaNP2
12040  -96076.1 * DeltaGF() / v() / v()
12041  -0.123 * deltaMwd6() )
12042  );
12043 
12044 // Linear contribution from Higgs self-coupling
12045  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
12046 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
12047  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
12048 
12049  // Add modifications due to small variations of the SM parameters
12050  dwidth += cHSM * ( +1. * deltaa0()
12051  -0.629 * deltaaMZ()
12052  +2.629 * deltaGmu()
12053  -4.926 * deltaMz()
12054  +0.004 * deltaaSMZ()
12055  +11.167 * deltaMh()
12056  +0.013 * deltamt()
12057  +0.004 * deltamb()
12058  +0.001 * deltamc()
12059  +0. * deltamtau() );
12060 
12061  // SM (1) + intrinsic + parametric theory relative errors (free pars)
12062  dwidth += eHZgaint + eHZgapar;
12063 
12064  return dwidth;
12065 }

◆ deltaGammaHZgaRatio2()

double NPSMEFTd6::deltaGammaHZgaRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z\gamma)\)/ \(\Gamma(H\to Z\gamma)_{\mathrm{SM}}\)

Definition at line 12067 of file NPSMEFTd6.cpp.

12068 {
12069  double dwidth = 0.0;
12070 
12071 
12072  //Contributions that are quadratic in the effective coefficients
12073  return ( dwidth );
12074 
12075 }

◆ deltaGammaHZllRatio1()

double NPSMEFTd6::deltaGammaHZllRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Zll)\)/ \(\Gamma(H\to Zll)_{\mathrm{SM}}\)

Definition at line 11181 of file NPSMEFTd6.cpp.

11182 {
11183  double dwidth = 0.0;
11184 
11185  double C1 = 0.0083;
11186 
11187  dwidth = ( +121715. * CiHbox / LambdaNP2
11188  +8726.9 * (1.0/2.0) * ( CiHL1_11 + CiHL1_22 ) / LambdaNP2
11189  -7315.2 * (1.0/2.0) * ( CiHe_11 + CiHe_22 ) / LambdaNP2
11190  +8726.9 * (1.0/2.0) * ( CiHL3_11 + CiHL3_22 ) / LambdaNP2
11191  -5544.15 * CiHD / LambdaNP2
11192  -13560.9 * CiHB / LambdaNP2
11193  -45585.2 * CiHW / LambdaNP2
11194  -53507.9 * CiHWB / LambdaNP2
11195  +16829.2 * CiDHB / LambdaNP2
11196  +30766.6 * CiDHW / LambdaNP2
11197  -2.204 * DeltaGF() );
11198 
11199 // Linear contribution from Higgs self-coupling
11200  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11201 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11202  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11203 
11204  // Add modifications due to small variations of the SM parameters
11205  //dwidth += cHSM * ( 0.0 );
11206 
11207  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11208  //dwidth += eHZZint + eHZZpar;
11209 
11210  return dwidth;
11211 
11212 }

◆ deltaGammaHZllRatio2()

double NPSMEFTd6::deltaGammaHZllRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Zll)\)/ \(\Gamma(H\to Zll)_{\mathrm{SM}}\)

Definition at line 11214 of file NPSMEFTd6.cpp.

11215 {
11216  double dwidth = 0.0;
11217 
11218 
11219  //Contributions that are quadratic in the effective coefficients
11220  return ( dwidth );
11221 
11222 }

◆ deltaGammaHZmumuRatio1()

double NPSMEFTd6::deltaGammaHZmumuRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z\mu\mu)\)/ \(\Gamma(H\to Z\mu\mu)_{\mathrm{SM}}\)

Definition at line 11301 of file NPSMEFTd6.cpp.

11302 {
11303  double dwidth = 0.0;
11304 
11305  double C1 = 0.0083;
11306 
11307 // Derived from the HZll expression for l=mu only
11308 
11309  dwidth = ( +121715. * CiHbox / LambdaNP2
11310  +8726.9 * CiHL1_22 / LambdaNP2
11311  -7315.2 * CiHe_22 / LambdaNP2
11312  +8726.9 * CiHL3_22 / LambdaNP2
11313  -5544.15 * CiHD / LambdaNP2
11314  -13560.9 * CiHB / LambdaNP2
11315  -45585.2 * CiHW / LambdaNP2
11316  -53507.9 * CiHWB / LambdaNP2
11317  +16829.2 * CiDHB / LambdaNP2
11318  +30766.6 * CiDHW / LambdaNP2
11319  -2.204 * DeltaGF() );
11320 
11321 // Linear contribution from Higgs self-coupling
11322  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11323 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11324  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11325 
11326  // Add modifications due to small variations of the SM parameters
11327  //dwidth += cHSM * ( 0.0 );
11328 
11329  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11330  //dwidth += eHZZint + eHZZpar;
11331 
11332  return dwidth;
11333 
11334 }

◆ deltaGammaHZmumuRatio2()

double NPSMEFTd6::deltaGammaHZmumuRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z\mu\mu)\)/ \(\Gamma(H\to Z\mu\mu)_{\mathrm{SM}}\)

Definition at line 11336 of file NPSMEFTd6.cpp.

11337 {
11338  double dwidth = 0.0;
11339 
11340 
11341  //Contributions that are quadratic in the effective coefficients
11342  return ( dwidth );
11343 
11344 }

◆ deltaGammaHZuuRatio1()

double NPSMEFTd6::deltaGammaHZuuRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z u u)\)/ \(\Gamma(H\to Z u u)_{\mathrm{SM}}\)

Definition at line 11741 of file NPSMEFTd6.cpp.

11742 {
11743  double dwidth = 0.0;
11744 
11745  double C1 = 0.0083;
11746 
11747  dwidth = ( +121512. * CiHbox / LambdaNP2
11748  -9648.28 * (1.0/2.0) * ( CiHQ1_11 + CiHQ1_22 ) / LambdaNP2
11749  +4218.6 * (1.0/2.0) * ( CiHu_11 + CiHu_22 ) / LambdaNP2
11750  +9648.28 * (1.0/2.0) * ( CiHQ3_11 + CiHQ3_22 ) / LambdaNP2
11751  -17762.5 * CiHD / LambdaNP2
11752  -13473.3 * CiHB / LambdaNP2
11753  -45667.9 * CiHW / LambdaNP2
11754  -110057. * CiHWB / LambdaNP2
11755  +16854.2 * CiDHB / LambdaNP2
11756  +30781.7 * CiDHW / LambdaNP2
11757  -2.6 * DeltaGF() );
11758 
11759 // Linear contribution from Higgs self-coupling
11760  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11761 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11762  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11763 
11764  // Add modifications due to small variations of the SM parameters
11765  //dwidth += cHSM * ( 0.0 );
11766 
11767  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11768  //dwidth += eHZZint + eHZZpar;
11769 
11770  return dwidth;
11771 
11772 }

◆ deltaGammaHZuuRatio2()

double NPSMEFTd6::deltaGammaHZuuRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z u u)\)/ \(\Gamma(H\to Z u u)_{\mathrm{SM}}\)

Definition at line 11774 of file NPSMEFTd6.cpp.

11775 {
11776  double dwidth = 0.0;
11777 
11778 
11779  //Contributions that are quadratic in the effective coefficients
11780  return ( dwidth );
11781 
11782 }

◆ deltaGammaHZvvRatio1()

double NPSMEFTd6::deltaGammaHZvvRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z\nu\nu)\)/ \(\Gamma(H\to Z\nu\nu)_{\mathrm{SM}}\)

Definition at line 11620 of file NPSMEFTd6.cpp.

11621 {
11622  double dwidth = 0.0;
11623 
11624  double C1 = 0.0083;
11625 
11626  dwidth = ( +121530. * CiHbox / LambdaNP2
11627  -7943.34 * (1.0/3.0) * ( CiHL1_11 + CiHL1_22 + CiHL1_33 ) / LambdaNP2
11628  +7943.34 * (1.0/3.0) * ( CiHL3_11 + CiHL3_22 + CiHL3_33 ) / LambdaNP2
11629  -229.41 * CiHD / LambdaNP2
11630  -13535.2 * CiHB / LambdaNP2
11631  -45480.6 * CiHW / LambdaNP2
11632  -24891. * CiHWB / LambdaNP2
11633  +16833. * CiDHB / LambdaNP2
11634  +30597.6 * CiDHW / LambdaNP2
11635  -2. * DeltaGF() );
11636 
11637 // Linear contribution from Higgs self-coupling
11638  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11639 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11640  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11641 
11642  // Add modifications due to small variations of the SM parameters
11643  //dwidth += cHSM * ( 0.0 );
11644 
11645  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11646  //dwidth += eHZZint + eHZZpar;
11647 
11648  return dwidth;
11649 
11650 }

◆ deltaGammaHZvvRatio2()

double NPSMEFTd6::deltaGammaHZvvRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z\nu\nu)\)/ \(\Gamma(H\to Z\nu\nu)_{\mathrm{SM}}\)

Definition at line 11652 of file NPSMEFTd6.cpp.

11653 {
11654  double dwidth = 0.0;
11655 
11656 
11657  //Contributions that are quadratic in the effective coefficients
11658  return ( dwidth );
11659 
11660 }

◆ deltaGammaHZZ2e2muRatio1()

double NPSMEFTd6::deltaGammaHZZ2e2muRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 2e2\mu)\)/ \(\Gamma(H\to ZZ* \to 2e2\mu)_{\mathrm{SM}}\)

Definition at line 11495 of file NPSMEFTd6.cpp.

11496 {
11497  double dwidth = 0.0;
11498 
11499  double C1 = 0.0083;
11500 
11501  dwidth = ( +120836. * CiHbox / LambdaNP2
11502  +126374. * (1.0/2.0) * ( CiHL1_11 + CiHL1_22 ) / LambdaNP2
11503  -109064. * (1.0/2.0) * ( CiHe_11 + CiHe_22 ) / LambdaNP2
11504  +126374. * (1.0/2.0) * ( CiHL3_11 + CiHL3_22 ) / LambdaNP2
11505  -42370.4 * CiHD / LambdaNP2
11506  -14299. * CiHB / LambdaNP2
11507  -47298.2 * CiHW / LambdaNP2
11508  -83098.2 * CiHWB / LambdaNP2
11509  +16362.7 * CiDHB / LambdaNP2
11510  +29503.4 * CiDHW / LambdaNP2
11511  -3.378 * DeltaGF()
11512  -0.85 * deltaGzd6() );
11513 
11514 // Linear contribution from Higgs self-coupling
11515  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11516 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11517  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11518 
11519  // Add modifications due to small variations of the SM parameters
11520  dwidth += cHSM * ( -10.07 * deltaMz()
11521  +15.626 * deltaMh()
11522  -0.128 * deltaaMZ()
11523  +2.258 * deltaGmu() );
11524 
11525  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11526  dwidth += eHZZint + eHZZpar;
11527 
11528  return dwidth;
11529 
11530 }

◆ deltaGammaHZZ2e2muRatio2()

double NPSMEFTd6::deltaGammaHZZ2e2muRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 2e2\mu)\)/ \(\Gamma(H\to ZZ* \to 2e2\mu)_{\mathrm{SM}}\)

Definition at line 11532 of file NPSMEFTd6.cpp.

11533 {
11534  double dwidth = 0.0;
11535 
11536  //Contributions that are quadratic in the effective coefficients
11537  return ( dwidth );
11538 
11539 }

◆ deltaGammaHZZ4dRatio1()

double NPSMEFTd6::deltaGammaHZZ4dRatio1 ( ) const
inline

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4 d)\)/ \(\Gamma(H\to ZZ* \to 4 d)_{\mathrm{SM}}\)

Definition at line 2463 of file NPSMEFTd6.h.

2464  {
2465  return 1.0;
2466  };

◆ deltaGammaHZZ4dRatio2()

double NPSMEFTd6::deltaGammaHZZ4dRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4 d)\)/ \(\Gamma(H\to ZZ* \to 4 d)_{\mathrm{SM}}\)

◆ deltaGammaHZZ4eRatio1()

double NPSMEFTd6::deltaGammaHZZ4eRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4e)\)/ \(\Gamma(H\to ZZ* \to 4e)_{\mathrm{SM}}\)

Definition at line 11432 of file NPSMEFTd6.cpp.

11433 {
11434  double dwidth = 0.0;
11435 
11436  double C1 = 0.0083;
11437 
11438  dwidth = ( +121386. * CiHbox / LambdaNP2
11439  +123413. * CiHL1_11 / LambdaNP2
11440  -103717. * CiHe_11 / LambdaNP2
11441  +123413. * CiHL3_11 / LambdaNP2
11442  -44056.9 * CiHD / LambdaNP2
11443  -13385.3 * CiHB / LambdaNP2
11444  -45127.7 * CiHW / LambdaNP2
11445  -91708.7 * CiHWB / LambdaNP2
11446  +16138.9 * CiDHB / LambdaNP2
11447  +28759.4 * CiDHW / LambdaNP2
11448  -3.462 * DeltaGF()
11449  -0.769 * deltaGzd6() );
11450 
11451 // Linear contribution from Higgs self-coupling
11452  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11453 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11454  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11455 
11456  // Add modifications due to small variations of the SM parameters
11457  dwidth += cHSM * ( -9.228 * deltaMz()
11458  +15.148 * deltaMh()
11459  -0.229 * deltaaMZ()
11460  +2.493 * deltaGmu() );
11461 
11462  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11463  dwidth += eHZZint + eHZZpar;
11464 
11465  return dwidth;
11466 
11467 }

◆ deltaGammaHZZ4eRatio2()

double NPSMEFTd6::deltaGammaHZZ4eRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4e)\)/ \(\Gamma(H\to ZZ* \to 4e)_{\mathrm{SM}}\)

Definition at line 11469 of file NPSMEFTd6.cpp.

11470 {
11471  double dwidth = 0.0;
11472 
11473 
11474  //Contributions that are quadratic in the effective coefficients
11475  return ( dwidth );
11476 
11477 }

◆ deltaGammaHZZ4fRatio1()

double NPSMEFTd6::deltaGammaHZZ4fRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4f)\)/ \(\Gamma(H\to ZZ* \to 4f)_{\mathrm{SM}}\)

Definition at line 11922 of file NPSMEFTd6.cpp.

11923 {
11924  double dwidth = 0.0;
11925 
11926  double C1 = 0.0083;
11927 
11928  double CZff, sf;
11929 
11930  CZff = gZvL*(-0.5 * (CiHL1_11 + CiHL1_22 + CiHL1_33 - CiHL3_11 - CiHL3_22 - CiHL3_33) * v2_over_LambdaNP2) +
11932  gZlR*(-0.5 * (CiHe_11 + CiHe_22 + CiHe_33) * v2_over_LambdaNP2) +
11933  Nc * (
11935  gZdR*(-0.5 * (CiHd_11 + CiHd_22 + CiHd_33) * v2_over_LambdaNP2) +
11937  gZuR*(-0.5 * (CiHu_11 + CiHu_22) * v2_over_LambdaNP2)
11938  );
11939 
11940  CZff = CZff/(
11941  3.0*( gZvL*gZvL + gZlL*gZlL + gZlR*gZlR ) +
11942  Nc * ( 3.0*( gZdL*gZdL + gZdR*gZdR ) + 2.0*( gZuL*gZuL + gZuR*gZuR ) )
11943  );
11944 
11945  sf = -11267.6 * (1.0/3.0) * (
11946  3.0*( gZvL*gZvL + gZlL*gZlL + gZlR*gZlR ) +
11947  Nc * ( 3.0*( gZdL*gZdL + gZdR*gZdR ) + 2.0*( gZuL*gZuL + gZuR*gZuR ) )
11948  );
11949 
11950  sf = sf/(-0.5*(gZlL + gZvL)*v2) ; // Coefficient of the CZff term. From the CiHL1_11 term in the ME.
11951 
11952  dwidth = ( +121373. * CiHbox / LambdaNP2
11953  + sf*CZff
11954  -50927.1 * CiHD / LambdaNP2
11955  -14137.9 * CiHB / LambdaNP2
11956  -46350.1 * CiHW / LambdaNP2
11957  -126336. * CiHWB / LambdaNP2
11958  +16558.7 * CiDHB / LambdaNP2
11959  +29628.7 * CiDHW / LambdaNP2
11960  -3.715 * DeltaGF()
11961  -0.834 * deltaGzd6()
11962  );
11963 
11964 // Linear contribution from Higgs self-coupling
11965  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11966 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11967  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11968 
11969  // Add modifications due to small variations of the SM parameters
11970  dwidth += cHSM * ( -9.548 * deltaMz()
11971  +15.799 * deltaMh()
11972  -0.412 * deltaaMZ()
11973  +2.569 * deltaGmu() );
11974 
11975  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11976  dwidth += eHZZint + eHZZpar;
11977 
11978  return dwidth;
11979 
11980 }

◆ deltaGammaHZZ4fRatio2()

double NPSMEFTd6::deltaGammaHZZ4fRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4f)\)/ \(\Gamma(H\to ZZ* \to 4f)_{\mathrm{SM}}\)

Definition at line 11982 of file NPSMEFTd6.cpp.

11983 {
11984  double dwidth = 0.0;
11985 
11986 
11987  //Contributions that are quadratic in the effective coefficients
11988  return ( dwidth );
11989 
11990 }

◆ deltaGammaHZZ4lRatio1()

double NPSMEFTd6::deltaGammaHZZ4lRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4l)\)/ \(\Gamma(H\to ZZ* \to 4l)_{\mathrm{SM}}\)

Definition at line 11362 of file NPSMEFTd6.cpp.

11363 {
11364  double dwidth = 0.0;
11365 
11366  double C1 = 0.0083;
11367 
11368  double CZll, sf;
11369 
11370  CZll = gZlL*(-0.5 * (CiHL1_11 + CiHL1_22 + CiHL3_11 + CiHL3_22) * v2_over_LambdaNP2) +
11371  gZlR*(-0.5 * (CiHe_11 + CiHe_22) * v2_over_LambdaNP2);
11372 
11373  CZll = CZll/(2.0*(gZlL*gZlL + gZlR*gZlR));
11374 
11375  sf = 124479. * (1.0/2.0) * (2.0*(gZlL*gZlL + gZlR*gZlR))/(-0.5*gZlL*v2) ; // Coefficient of the CZll term. From the CiHL1_11 term in the ME.
11376 
11377  dwidth = ( +122273. * CiHbox / LambdaNP2
11378  + sf*CZll
11379  -44025.7 * CiHD / LambdaNP2
11380  -13602.6 * CiHB / LambdaNP2
11381  -45248.6 * CiHW / LambdaNP2
11382  -88372.1 * CiHWB / LambdaNP2
11383  +16088.6 * CiDHB / LambdaNP2
11384  +29210.1 * CiDHW / LambdaNP2
11385  -3.462 * DeltaGF()
11386  -0.808 * deltaGzd6() );
11387 
11388 // Linear contribution from Higgs self-coupling
11389  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11390 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11391  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11392 
11393  // Add modifications due to small variations of the SM parameters
11394  dwidth += cHSM * ( -9.734 * deltaMz()
11395  +15.37 * deltaMh()
11396  -0.154 * deltaaMZ()
11397  +2.339 * deltaGmu() );
11398 
11399  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11400  dwidth += eHZZint + eHZZpar;
11401 
11402  return dwidth;
11403 
11404 }

◆ deltaGammaHZZ4lRatio2()

double NPSMEFTd6::deltaGammaHZZ4lRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4l)\)/ \(\Gamma(H\to ZZ* \to 4l)_{\mathrm{SM}}\)

Definition at line 11406 of file NPSMEFTd6.cpp.

11407 {
11408  double dwidth = 0.0;
11409 
11410 
11411  //Contributions that are quadratic in the effective coefficients
11412  return ( dwidth );
11413 
11414 }

◆ deltaGammaHZZ4muRatio1()

double NPSMEFTd6::deltaGammaHZZ4muRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4\mu)\)/ \(\Gamma(H\to ZZ* \to 4\mu)_{\mathrm{SM}}\)

Definition at line 11557 of file NPSMEFTd6.cpp.

11558 {
11559  double dwidth = 0.0;
11560 
11561  double C1 = 0.0083;
11562 
11563  dwidth = ( +120688. * CiHbox / LambdaNP2
11564  +123059. * CiHL1_22 / LambdaNP2
11565  -103862. * CiHe_22 / LambdaNP2
11566  +123059. * CiHL3_22 / LambdaNP2
11567  -43977.1 * CiHD / LambdaNP2
11568  -13575.5 * CiHB / LambdaNP2
11569  -45200.8 * CiHW / LambdaNP2
11570  -91625.2 * CiHWB / LambdaNP2
11571  +15449.3 * CiDHB / LambdaNP2
11572  +28489.5 * CiDHW / LambdaNP2
11573  -3.471 * DeltaGF()
11574  -0.774 * deltaGzd6() );
11575 
11576 // Linear contribution from Higgs self-coupling
11577  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11578 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11579  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11580 
11581  // Add modifications due to small variations of the SM parameters
11582  dwidth += cHSM * ( -9.254 * deltaMz()
11583  +15.109 * deltaMh()
11584  -0.207 * deltaaMZ()
11585  +2.405 * deltaGmu() );
11586 
11587  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11588  dwidth += eHZZint + eHZZpar;
11589 
11590  return dwidth;
11591 
11592 }

◆ deltaGammaHZZ4muRatio2()

double NPSMEFTd6::deltaGammaHZZ4muRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4\mu)\)/ \(\Gamma(H\to ZZ* \to 4\mu)_{\mathrm{SM}}\)

Definition at line 11594 of file NPSMEFTd6.cpp.

11595 {
11596  double dwidth = 0.0;
11597 
11598 
11599  //Contributions that are quadratic in the effective coefficients
11600  return ( dwidth );
11601 
11602 }

◆ deltaGammaHZZ4uRatio1()

double NPSMEFTd6::deltaGammaHZZ4uRatio1 ( ) const
inline

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4 u)\)/ \(\Gamma(H\to ZZ* \to 4 u)_{\mathrm{SM}}\)

Definition at line 2446 of file NPSMEFTd6.h.

2447  {
2448  return 1.0;
2449  };

◆ deltaGammaHZZ4uRatio2()

double NPSMEFTd6::deltaGammaHZZ4uRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4 u)\)/ \(\Gamma(H\to ZZ* \to 4 u)_{\mathrm{SM}}\)

◆ deltaGammaHZZ4vRatio1()

double NPSMEFTd6::deltaGammaHZZ4vRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4\nu)\)/ \(\Gamma(H\to ZZ* \to 4\nu)_{\mathrm{SM}}\)

Definition at line 11678 of file NPSMEFTd6.cpp.

11679 {
11680  double dwidth = 0.0;
11681 
11682  double C1 = 0.0083;
11683 
11684  dwidth = ( +120596. * CiHbox / LambdaNP2
11685  -115532. * (1.0/3.0) * ( CiHL1_11 + CiHL1_22 + CiHL1_33 ) / LambdaNP2
11686  +115532. * (1.0/3.0) * ( CiHL3_11 + CiHL3_22 + CiHL3_33 ) / LambdaNP2
11687  -28744.1 * CiHD / LambdaNP2
11688  -13816.7 * CiHB / LambdaNP2
11689  -44782.1 * CiHW / LambdaNP2
11690  -25256.6 * CiHWB / LambdaNP2
11691  +15982.5 * CiDHB / LambdaNP2
11692  +28910.7 * CiDHW / LambdaNP2
11693  -3.013 * DeltaGF()
11694  -0.787 * deltaGzd6()
11695  );
11696 
11697 // Linear contribution from Higgs self-coupling
11698  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11699 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11700  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11701 
11702  // Add modifications due to small variations of the SM parameters
11703  dwidth += cHSM * ( -10.49 * deltaMz()
11704  +15.294 * deltaMh()
11705  +0.255 * deltaaMZ()
11706  +1.979 * deltaGmu() );
11707 
11708  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11709  dwidth += eHZZint + eHZZpar;
11710 
11711  return dwidth;
11712 
11713 }

◆ deltaGammaHZZ4vRatio2()

double NPSMEFTd6::deltaGammaHZZ4vRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4\nu)\)/ \(\Gamma(H\to ZZ* \to 4\nu)_{\mathrm{SM}}\)

Definition at line 11715 of file NPSMEFTd6.cpp.

11716 {
11717  double dwidth = 0.0;
11718 
11719 
11720  //Contributions that are quadratic in the effective coefficients
11721  return ( dwidth );
11722 
11723 }

◆ deltaGammaHZZRatio1()

double NPSMEFTd6::deltaGammaHZZRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ)\)/ \(\Gamma(H\to ZZ)_{\mathrm{SM}}\)

Definition at line 11133 of file NPSMEFTd6.cpp.

11134 {
11135  double dwidth = 0.0;
11136 
11137 // double C1 = 0.0083;
11138 
11139  dwidth = deltaGammaHZZ4fRatio1();
11140 
11141 // Linear contribution from Higgs self-coupling
11142 // dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11143 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11144 // dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11145 
11146  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11147 // dwidth += eHZZint + eHZZpar;
11148 
11149  return dwidth;
11150 
11151 }

◆ deltaGammaHZZRatio2()

double NPSMEFTd6::deltaGammaHZZRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ)\)/ \(\Gamma(H\to ZZ)_{\mathrm{SM}}\)

Definition at line 11153 of file NPSMEFTd6.cpp.

11154 {
11155  double dwidth = 0.0;
11156 
11157  //Contributions that are quadratic in the effective coefficients
11158  dwidth = deltaGammaHZZ4fRatio2();
11159 
11160 
11161  return dwidth;
11162 
11163 }

◆ deltaGammaTotalRatio1()

double NPSMEFTd6::deltaGammaTotalRatio1 ( ) const
virtual

The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients.

Returns
\(\delta \Gamma(H)\)/ \(\Gamma(H)_{\mathrm{SM}}\)

Definition at line 10585 of file NPSMEFTd6.cpp.

10586 {
10587  double deltaGammaRatio;
10588 
10589 // The change in the ratio asumming only SM decays
10590  deltaGammaRatio = ( trueSM.computeBrHtogg() * deltaGammaHggRatio1()
10599 
10600 // Add the effect of the invisible and exotic BR. Include also here the
10601 // pure contribution from BrHinv and BrHexo even in case of no dim 6 contibutions
10602  deltaGammaRatio = -1.0 + (1.0 + deltaGammaRatio) / (1.0 - BrHinv - BrHexo);
10603 
10604  return deltaGammaRatio;
10605 }

◆ deltaGammaTotalRatio1noError()

double NPSMEFTd6::deltaGammaTotalRatio1noError ( ) const
virtual

The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. Neglecting SM theory errors.

Returns
\(\delta \Gamma(H)\)/ \(\Gamma(H)_{\mathrm{SM}}\)

Definition at line 10607 of file NPSMEFTd6.cpp.

10608 {
10609  double deltaGammaRatio;
10610 
10611 // The change in the ratio asumming only SM decays
10612  deltaGammaRatio = ( trueSM.computeBrHtogg() * (deltaGammaHggRatio1() - eHggint - eHggpar )
10621 
10622 // Add the effect of the invisible and exotic BR. Include also here the
10623 // pure contribution from BrHinv and BrHexo even in case of no dim 6 contibutions
10624  deltaGammaRatio = -1.0 + (1.0 + deltaGammaRatio) / (1.0 - BrHinv - BrHexo);
10625 
10626  return deltaGammaRatio;
10627 }

◆ deltaGammaTotalRatio2()

double NPSMEFTd6::deltaGammaTotalRatio2 ( ) const
virtual

The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are quadratic in the effective Lagrangian coefficients.

Returns
\(\delta \Gamma(H)\)/ \(\Gamma(H)_{\mathrm{SM}}\)

Definition at line 10629 of file NPSMEFTd6.cpp.

10630 {
10631  double deltaGammaRatio;
10632 
10633 // The change in the ratio asumming only SM decays
10634  deltaGammaRatio = trueSM.computeBrHtogg() * deltaGammaHggRatio2()
10643 
10644 // Add the effect of the invisible and exotic BR and return
10645  return (deltaGammaRatio / (1.0 - BrHinv - BrHexo));
10646 }

◆ DeltaGF()

double NPSMEFTd6::DeltaGF ( ) const
virtual

New physics contribution to the Fermi constant.

The new physics contribution \(\Delta G\) is defined as

\[ G_\mu = G_{\mu,\mathrm{SM}}(1+\Delta G)\,, \]

where \(G_\mu\) is the experimental value measured through muon decays, and \(G_{\mu,\mathrm{SM}}\) is the Fermi constant in the SM.

Returns
\(\Delta G\)

Reimplemented from NPbase.

Definition at line 2598 of file NPSMEFTd6.cpp.

2599 {
2600  return ((CiHL3_11 + CiHL3_22 - 0.5 * (CiLL_1221 + CiLL_2112)) * v2_over_LambdaNP2);
2601 }

◆ deltaGL_f()

double NPSMEFTd6::deltaGL_f ( const Particle  p) const

New physics contribution to the neutral-current left-handed coupling \(g_L^f\).

Parameters
[in]fa lepton or quark
Returns
\(\delta g_L^f\)

Definition at line 2852 of file NPSMEFTd6.cpp.

2853 {
2854  double I3p = p.getIsospin(), Qp = p.getCharge();
2855  double CHF1 = CHF1_diag(p);
2856  double CHF3 = CHF3_diag(p);
2857  double NPindirect;
2858 
2859  NPindirect = -I3p / 4.0 * (CiHD * v2_over_LambdaNP2 + 2.0 * DeltaGF())
2860  - Qp * sW2_tree / 4.0 / (cW2_tree - sW2_tree)
2861  *((4.0 * cW_tree / sW_tree * CiHWB + CiHD) * v2_over_LambdaNP2 + 2.0 * DeltaGF());
2862 
2863  double NPdirect = -0.5 * (CHF1 - 2.0 * I3p * CHF3) * v2_over_LambdaNP2;
2864  return (NPindirect + NPdirect);
2865 }

◆ deltaGL_Wff()

gslpp::complex NPSMEFTd6::deltaGL_Wff ( const Particle  pbar,
const Particle  p 
) const
virtual

New physics contribution to the charged current coupling \(W_\mu \bar{f_L}\gamma^mu f_L\).

Parameters
[in]pbara lepton or quark
[in]pa lepton or quark
Returns
\(\delta g_{Wff}^{L}\)

Reimplemented from NPbase.

Definition at line 2883 of file NPSMEFTd6.cpp.

2884 {
2885  if (pbar.getIndex() + 1 != p.getIndex() || pbar.getIndex() % 2 != 0)
2886  throw std::runtime_error("NPSMEFTd6::deltaGL_Wff(): Not implemented");
2887 
2888  double CHF3 = CHF3_diag(pbar);
2889  double NPindirect;
2890 
2891  NPindirect = -cW2_tree / 4.0 / (cW2_tree - sW2_tree)
2892  * ((4.0 * sW_tree / cW_tree * CiHWB + CiHD) * v2_over_LambdaNP2 + 2.0 * DeltaGF());
2893 
2894  double NPdirect = CHF3 * v2_over_LambdaNP2;
2895  return (NPindirect + NPdirect);
2896 }

◆ deltaGL_Wffh()

gslpp::complex NPSMEFTd6::deltaGL_Wffh ( const Particle  pbar,
const Particle  p 
) const

The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_L}\gamma^mu f_L\).

Parameters
[in]pbara lepton or quark
[in]pa lepton or quark
Returns
\(\delta g_{WffH}^{L}\)

Definition at line 3143 of file NPSMEFTd6.cpp.

3144 {
3145  if (pbar.getIndex() + 1 != p.getIndex() || pbar.getIndex() % 2 != 0)
3146  throw std::runtime_error("NPSMEFTd6::deltaGL_Wffh(): Not implemented");
3147 
3148  double CHF3 = CHF3_diag(pbar);
3149  return (2.0 * sqrt(2.0) * Mz * cW_tree / v() / v() * CHF3 * v2_over_LambdaNP2);
3150 }

◆ deltaGL_Zffh()

double NPSMEFTd6::deltaGL_Zffh ( const Particle  p) const

The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_L}\gamma^mu f_L\).

Parameters
[in]pa lepton or quark
Returns
\(\delta g_{ZffH}^{L}\)

Definition at line 3161 of file NPSMEFTd6.cpp.

3162 {
3163  double I3p = p.getIsospin();
3164  double CHF1 = CHF1_diag(p);
3165  double CHF3 = CHF3_diag(p);
3166  return (-2.0 * Mz / v() / v() * (CHF1 - 2.0 * I3p * CHF3) * v2_over_LambdaNP2);
3167 }

◆ deltaGmu()

double NPSMEFTd6::deltaGmu ( ) const
virtual

The relative correction to the muon decay constant, \(\delta G_\mu/G_\mu\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\(\delta G_\mu/G_\mu\)

Definition at line 2696 of file NPSMEFTd6.cpp.

2697 {
2698  // Ref. value fixed in SM EW fit 2018: from PDG 2018
2699  return ( (GF - 1.1663787/100000.0 ) / (1.1663787/100000.0) );
2700 }

◆ deltaGmu2()

double NPSMEFTd6::deltaGmu2 ( ) const
virtual

The relative correction to the muon decay constant, \((\delta G_\mu/G_\mu)^2\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\((\delta G_\mu/G_\mu)^2\)

Definition at line 2702 of file NPSMEFTd6.cpp.

2703 {
2704  return ( 0.0 );
2705 }

◆ deltaGR_f()

double NPSMEFTd6::deltaGR_f ( const Particle  p) const

New physics contribution to the neutral-current right-handed coupling \(g_R^f\).

Parameters
[in]fa lepton or quark
Returns
\(\delta g_R^f\)

Definition at line 2867 of file NPSMEFTd6.cpp.

2868 {
2869  double Qp = p.getCharge();
2870  double CHf = CHf_diag(p);
2871  double NPindirect;
2872 
2873  NPindirect = -Qp * sW2_tree / 4.0 / (cW2_tree - sW2_tree)
2874  *((4.0 * cW_tree / sW_tree * CiHWB + CiHD) * v2_over_LambdaNP2 + 2.0 * DeltaGF());
2875 
2876  double NPdirect = -0.5 * CHf*v2_over_LambdaNP2;
2877  return (NPindirect + NPdirect);
2878 }

◆ deltaGR_Wff()

gslpp::complex NPSMEFTd6::deltaGR_Wff ( const Particle  pbar,
const Particle  p 
) const
virtual

New physics contribution to the charged current coupling \(W_\mu \bar{f_R}\gamma^mu f_R\).

Parameters
[in]pbara lepton or quark
[in]pa lepton or quark
Returns
\(\delta g_{Wff}^{R}\)

Reimplemented from NPbase.

Definition at line 2898 of file NPSMEFTd6.cpp.

2899 {
2900  if (pbar.getIndex() + 1 != p.getIndex() || pbar.getIndex() % 2 != 0)
2901  throw std::runtime_error("NPSMEFTd6::deltaGR_Wff(): Not implemented");
2902 
2903  gslpp::complex CHud = CHud_diag(pbar);
2904  return (0.5 * CHud * v2_over_LambdaNP2);
2905 }

◆ deltaGR_Wffh()

gslpp::complex NPSMEFTd6::deltaGR_Wffh ( const Particle  pbar,
const Particle  p 
) const

The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_R}\gamma^mu f_R\).

Parameters
[in]pbara lepton or quark
[in]pa lepton or quark
Returns
\(\delta g_{WffH}^{R}\)

Definition at line 3152 of file NPSMEFTd6.cpp.

3153 {
3154  if (pbar.getIndex() + 1 != p.getIndex() || pbar.getIndex() % 2 != 0)
3155  throw std::runtime_error("NPSMEFTd6::deltaGR_Wffh(): Not implemented");
3156 
3157  gslpp::complex CHud = CHud_diag(pbar);
3158  return (sqrt(2.0) * Mz * cW_tree / v() / v() * CHud * v2_over_LambdaNP2);
3159 }

◆ deltaGR_Zffh()

double NPSMEFTd6::deltaGR_Zffh ( const Particle  p) const

The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_R}\gamma^mu f_R\).

Parameters
[in]pa lepton or quark
Returns
\(\delta g_{ZffH}^{R}\)

Definition at line 3169 of file NPSMEFTd6.cpp.

3170 {
3171  double CHf = CHf_diag(p);
3172  return (-2.0 * Mz / v() / v() * CHf * v2_over_LambdaNP2);
3173 }

◆ deltaGV_f()

double NPSMEFTd6::deltaGV_f ( const Particle  p) const
virtual

New physics contribution to the neutral-current vector coupling \(g_V^f\).

Parameters
[in]fa lepton or quark
Returns
\(\delta g_V^f\)

Reimplemented from NPbase.

Definition at line 2842 of file NPSMEFTd6.cpp.

2843 {
2844  return (deltaGL_f(p) + deltaGR_f(p));
2845 }

◆ deltaGwd6()

double NPSMEFTd6::deltaGwd6 ( ) const
virtual

The relative NP corrections to the width of the \(W\) boson, \(\delta \Gamma_W/\Gamma_W\).

Returns
\(\delta \Gamma_W/\Gamma_W\)

Definition at line 2818 of file NPSMEFTd6.cpp.

2819 {
2820  return ( deltaGamma_W() / trueSM.GammaW() );
2821 }

◆ deltaGwd62()

double NPSMEFTd6::deltaGwd62 ( ) const
virtual

The relative NP corrections to the width of the \(W\) boson squared, \((\delta \Gamma_W/\Gamma_W)^2\).

Returns
\((\delta \Gamma_W/\Gamma_W)^2\)

Definition at line 2823 of file NPSMEFTd6.cpp.

2824 {
2825  double dWW = 0.0;
2826 
2827  return (dWW*dWW);
2828 }

◆ deltaGzd6()

double NPSMEFTd6::deltaGzd6 ( ) const
virtual

The relative NP corrections to the width of the \(Z\) boson, \(\delta \Gamma_Z/\Gamma_Z\).

Returns
\(\delta \Gamma_Z/\Gamma_Z\)

Definition at line 2830 of file NPSMEFTd6.cpp.

2831 {
2832  return ( deltaGamma_Z() / trueSM.Gamma_Z() );
2833 }

◆ deltaGzd62()

double NPSMEFTd6::deltaGzd62 ( ) const
virtual

The relative NP corrections to the width of the \(Z\) boson squared, \((\delta \Gamma_Z/\Gamma_Z)^2\).

Returns
\((\delta \Gamma_Z/\Gamma_Z)^2\)

Definition at line 2835 of file NPSMEFTd6.cpp.

2836 {
2837  double dWZ = 0.0;
2838 
2839  return (dWZ*dWZ);
2840 }

◆ deltaKgammaNP()

double NPSMEFTd6::deltaKgammaNP ( ) const
virtual

The new physics contribution to the anomalous triple gauge coupling \(\kappa_{\gamma}\).

Returns
\(\delta \kappa_{\gamma}\)

Reimplemented from NPbase.

Definition at line 13512 of file NPSMEFTd6.cpp.

13513 {
13514  double NPdirect;
13515 
13516  /* Translate from LHCHXWG-INT-2015-001: Checked with own calculations */
13517  NPdirect = sqrt( 4.0 * M_PI * aleMz ) / 4.0 / sW2_tree;
13518 
13519  NPdirect = NPdirect * ( (4.0 * sW_tree * cW_tree / sqrt( 4.0 * M_PI * aleMz ) ) * CiHWB
13520  - sW_tree * CiDHW
13522 
13523  return NPdirect + dKappaga ;
13524 }

◆ deltaKgammaNPEff()

double NPSMEFTd6::deltaKgammaNPEff ( ) const
virtual

The new physics contribution to the effective anomalous triple gauge coupling \(\kappa_{\gamma}^{Eff}\) from arXiv: 1708.09079 [hep-ph].

Returns
\(\delta \kappa_{\gamma}\)

Reimplemented from NPbase.

Definition at line 13551 of file NPSMEFTd6.cpp.

13552 {
13553  /* From arXiv:1708.09079 [hep-ph]. In our case, delta_e=0 since it is taken as inputs and its effects propagated
13554  * everywhere else */
13555  double dgEff;
13556 
13559 
13560  return dgEff + deltaKgammaNP() ;
13561 }

◆ deltamb()

double NPSMEFTd6::deltamb ( ) const
virtual

The relative correction to the mass of the \(b\) quark, \(\delta m_b/m_b\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\(\delta m_b/m_b\)

Definition at line 2663 of file NPSMEFTd6.cpp.

2664 {
2665  // Ref. value fixed in SM EW fit 2018: from PDG 2018
2666  return ( ((quarks[BOTTOM].getMass()) - 4.18) / 4.18 );
2667 }

◆ deltamb2()

double NPSMEFTd6::deltamb2 ( ) const
virtual

The relative correction to the mass of the \(b\) quark squared, \((\delta m_b/m_b)^2\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\((\delta m_b/m_b)^2\)

Definition at line 2669 of file NPSMEFTd6.cpp.

2670 {
2671  return ( 0.0 );
2672 }

◆ deltamc()

double NPSMEFTd6::deltamc ( ) const
virtual

The relative correction to the mass of the \(c\) quark, \(\delta m_c/m_c\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\(\delta m_c/m_c\)

Definition at line 2674 of file NPSMEFTd6.cpp.

2675 {
2676  // Ref. value fixed in SM EW fit 2018: from PDG 2018
2677  return ( ((quarks[CHARM].getMass()) - 1.275) / 1.275 );
2678 }

◆ deltamc2()

double NPSMEFTd6::deltamc2 ( ) const
virtual

The relative correction to the mass of the \(c\) quark squared, \((\delta m_c/m_c)^2\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\((\delta m_c/m_c)^2\)

Definition at line 2680 of file NPSMEFTd6.cpp.

2681 {
2682  return ( 0.0 );
2683 }

◆ deltaMh()

double NPSMEFTd6::deltaMh ( ) const
virtual

The relative correction to the mass of the \(H\) boson, \(\delta M_H/M_H\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\(\delta M_H/M_H\)

Definition at line 2641 of file NPSMEFTd6.cpp.

2642 {
2643  // Ref. value from SM EW fit 2018
2644  return ( (mHl - 125.1) / 125.1 );
2645 }

◆ deltaMh2()

double NPSMEFTd6::deltaMh2 ( ) const
virtual

The relative correction to the mass of the \(H\) boson squared, \((\delta M_H/M_H)^2\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\((\delta M_H/M_H)^2\)

Definition at line 2647 of file NPSMEFTd6.cpp.

2648 {
2649  return ( 0.0 );
2650 }

◆ deltamt()

double NPSMEFTd6::deltamt ( ) const
virtual

The relative correction to the mass of the \(t\) quark, \(\delta m_t/m_t\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\(\delta m_t/m_t\)

Definition at line 2652 of file NPSMEFTd6.cpp.

2653 {
2654  // Ref. value from SM EW fit 2018
2655  return ( (mtpole - 173.2) / 173.2 );
2656 }

◆ deltamt2()

double NPSMEFTd6::deltamt2 ( ) const
virtual

The relative correction to the mass of the \(t\) quark squared, \((\delta m_t/m_t)^2\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\((\delta m_t/m_t)^2\)

Definition at line 2658 of file NPSMEFTd6.cpp.

2659 {
2660  return ( 0.0 );
2661 }

◆ deltamtau()

double NPSMEFTd6::deltamtau ( ) const
virtual

The relative correction to the mass of the \(\tau\) lepton, \(\delta m_\tau/m_\tau\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\(\delta m_\tau/m_\tau\)

Definition at line 2685 of file NPSMEFTd6.cpp.

2686 {
2687  // Ref. value fixed in SM EW fit 2018: from PDG 2018
2688  return ( ((leptons[TAU].getMass()) - 1.77686) / 1.77686 );
2689 }

◆ deltamtau2()

double NPSMEFTd6::deltamtau2 ( ) const
virtual

The relative correction to the mass of the \(\tau\) lepton squared, \((\delta m_\tau/m_\tau)^2\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\((\delta m_\tau/m_\tau)^2\)

Definition at line 2691 of file NPSMEFTd6.cpp.

2692 {
2693  return ( 0.0 );
2694 }

◆ deltaMwd6()

double NPSMEFTd6::deltaMwd6 ( ) const
virtual

The relative NP corrections to the mass of the \(W\) boson, \(\delta M_W/M_W\).

Returns
\(\delta M_W/M_W\)

Definition at line 2751 of file NPSMEFTd6.cpp.

2752 {
2753  return (- 1.0 / 4.0 / (cW2_tree - sW2_tree)
2754  *(4.0 * sW_tree * cW_tree * CiHWB * v2_over_LambdaNP2
2756  + 2.0 * sW2_tree * DeltaGF()));
2757 }

◆ deltaMwd62()

double NPSMEFTd6::deltaMwd62 ( ) const
virtual

The relative NP corrections to the mass of the \(W\) boson squared, \((\delta M_W/M_W)^2\).

Returns
\((\delta M_W/M_W)^2\)

Definition at line 2759 of file NPSMEFTd6.cpp.

2760 {
2761  double dMW = 0.0;
2762 
2763  return (dMW*dMW);
2764 }

◆ deltaMz()

double NPSMEFTd6::deltaMz ( ) const
virtual

The relative correction to the mass of the \(Z\) boson, \(\delta M_Z/M_Z\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\(\delta M_Z/M_Z\)

Definition at line 2630 of file NPSMEFTd6.cpp.

2631 {
2632  // Ref. value from SM EW fit 2018
2633  return ( (Mz - 91.1882) / 91.1882 );
2634 }

◆ deltaMz2()

double NPSMEFTd6::deltaMz2 ( ) const
virtual

The relative correction to the mass of the \(Z\) boson squared, \((\delta M_Z/M_Z)^2\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\((\delta M_Z/M_Z)^2\)

Definition at line 2636 of file NPSMEFTd6.cpp.

2637 {
2638  return ( 0.0 );
2639 }

◆ deltayb_HB()

double NPSMEFTd6::deltayb_HB ( ) const
virtual

The Higgs-basis coupling \(\delta y_b\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(\delta y_b\)

Reimplemented from NPbase.

Definition at line 15156 of file NPSMEFTd6.cpp.

15157 {
15158  double mf= (quarks[BOTTOM].getMass());
15159  double ciHB;
15160 
15161  ciHB = - (v()/mf/sqrt(2.0))*CidH_33r*v2_over_LambdaNP2 + delta_h - 0.5*DeltaGF();
15162 
15163  return ciHB;
15164 }

◆ deltayc_HB()

double NPSMEFTd6::deltayc_HB ( ) const
virtual

The Higgs-basis coupling \(\delta y_c\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(\delta y_c\)

Reimplemented from NPbase.

Definition at line 15178 of file NPSMEFTd6.cpp.

15179 {
15180  double mf= (quarks[CHARM].getMass());
15181  double ciHB;
15182 
15183  ciHB = - (v()/mf/sqrt(2.0))*CiuH_22r*v2_over_LambdaNP2 + delta_h - 0.5*DeltaGF();
15184 
15185  return ciHB;
15186 }

◆ deltaymu_HB()

double NPSMEFTd6::deltaymu_HB ( ) const
virtual

The Higgs-basis coupling \(\delta y_\mu\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(\delta y_\mu\)

Reimplemented from NPbase.

Definition at line 15189 of file NPSMEFTd6.cpp.

15190 {
15191  double mf= (leptons[MU].getMass());
15192  double ciHB;
15193 
15194  ciHB = - (v()/mf/sqrt(2.0))*CieH_22r*v2_over_LambdaNP2 + delta_h - 0.5*DeltaGF();
15195 
15196  return ciHB;
15197 }

◆ deltayt_HB()

double NPSMEFTd6::deltayt_HB ( ) const
virtual

The Higgs-basis coupling \(\delta y_t\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(\delta y_t\)

Reimplemented from NPbase.

Definition at line 15145 of file NPSMEFTd6.cpp.

15146 {
15147  double mf= mtpole;
15148  double ciHB;
15149 
15150  ciHB = - (v()/mf/sqrt(2.0))*CiuH_33r*v2_over_LambdaNP2 + delta_h - 0.5*DeltaGF();
15151 
15152  return ciHB;
15153 }

◆ deltaytau_HB()

double NPSMEFTd6::deltaytau_HB ( ) const
virtual

The Higgs-basis coupling \(\delta y_\tau\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(\delta y_\tau\)

Reimplemented from NPbase.

Definition at line 15167 of file NPSMEFTd6.cpp.

15168 {
15169  double mf= (leptons[TAU].getMass());
15170  double ciHB;
15171 
15172  ciHB = - (v()/mf/sqrt(2.0))*CieH_33r*v2_over_LambdaNP2 + delta_h - 0.5*DeltaGF();
15173 
15174  return ciHB;
15175 }

◆ dxseeWWdcos()

double NPSMEFTd6::dxseeWWdcos ( const double  sqrt_s,
const double  cos 
) const
virtual

The differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\), as a function of the \(W\) polar angle.

Returns
\(d\sigma/d\cos{\theta}\)

Reimplemented from NPbase.

Definition at line 13565 of file NPSMEFTd6.cpp.

13566 {
13567  double sqrt_sGeV = 1000. * sqrt_s;
13568  double s = sqrt_sGeV * sqrt_sGeV;
13569  double cos2 = cos * cos;
13570  double sin2 = 1.0 - cos2;
13571  double sin = sqrt(sin2);
13572 
13573  double topb = 0.3894*1000000000.0;
13574 
13575 // NC and CC couplings
13576  double gLe, gRe;
13577  gslpp::complex Uenu;
13578 
13579  gLe = -0.5 + sW2_tree + deltaGL_f(leptons[ELECTRON]);
13580  gRe = sW2_tree + deltaGR_f(leptons[ELECTRON]);
13581 
13583  Uenu = 1.0 + Uenu;
13584 
13585 // W mass
13586  double mw;
13587 
13588  mw = Mw();
13589 
13590 // Wigner functions
13591  double d1pp[2],d1mm[2],d1p0[2],d1m0[2],d10p[2],d10m[2],d100[2];
13592 
13593  d1pp[0]=sqrt((1.0 - cos2)/2.0);
13594  d1pp[1]=-sqrt((1.0 - cos2)/2.0);
13595 
13596  d1mm[0]=d1pp[0];
13597  d1mm[1]=d1pp[1];
13598 
13599  d1p0[0]=(1.0 - cos)/2.0;
13600  d1p0[1]=(1.0 + cos)/2.0;
13601 
13602  d1m0[0]=d1p0[1];
13603  d1m0[1]=d1p0[0];
13604 
13605  d10p[0]=d1p0[1];
13606  d10p[1]=d1p0[0];
13607 
13608  d10m[0]=d1p0[0];
13609  d10m[1]=d1p0[1];
13610 
13611  d100[0]=d1pp[0];
13612  d100[1]=d1pp[1];
13613 
13614  gslpp::matrix<double> d1LH(3, 3, 0.0);
13615 
13616  gslpp::matrix<double> d1RH(3, 3, 0.0);
13617 
13618  d1LH.assign(0,0, d1pp[0]);
13619  d1LH.assign(0,1, d1p0[0]);
13620  d1LH.assign(0,2, 0.0);
13621 
13622  d1LH.assign(1,0, d10p[0]);
13623  d1LH.assign(1,1, d100[0]);
13624  d1LH.assign(1,2, d10m[0]);
13625 
13626  d1LH.assign(2,0, 0.0);
13627  d1LH.assign(2,1, d1m0[0]);
13628  d1LH.assign(2,2, d1mm[0]);
13629 
13630  d1RH.assign(0,0, d1pp[1]);
13631  d1RH.assign(0,1, d1p0[1]);
13632  d1RH.assign(0,2, 0.0);
13633 
13634  d1RH.assign(1,0, d10p[1]);
13635  d1RH.assign(1,1, d100[1]);
13636  d1RH.assign(1,2, d10m[1]);
13637 
13638  d1RH.assign(2,0, 0.0);
13639  d1RH.assign(2,1, d1m0[1]);
13640  d1RH.assign(2,2, d1mm[1]);
13641 
13642 // TGC parameterization
13643  double g1Z,g1ga,kZ,kga,lambdaZ,lambdaga,g4Z,g4ga,g5Z,g5ga,ktZ,ktga,lambdatZ,lambdatga;
13644 
13645 // TGC present in the SM
13646  g1Z=1.0 + deltag1ZNP();
13647  g1ga=1.0;
13648  kZ=1.0 + deltag1ZNP() - (sW2_tree/cW2_tree) * deltaKgammaNP();
13649  kga=1.0 + deltaKgammaNP();
13650 // TGC not present in the SM
13651  lambdaZ=lambdaZNP(); //Check normalization
13652  lambdaga=lambdaZ;
13653  g4Z=0.0;
13654  g4ga=0.0;
13655  g5Z=0.0;
13656  g5ga=0.0;
13657  ktZ=0.0;
13658  ktga=0.0;
13659  lambdatZ=0.0;
13660  lambdatga=0.0;
13661 
13662  double f3Z, f3ga;
13663 
13664  f3Z = g1Z + kZ + lambdaZ;
13665  f3ga = g1ga + kga + lambdaga;
13666 
13667  // Kinematic factors
13668  double beta, gamma, gamma2;
13669 
13670  beta = sqrt(1.0 - 4.0 * mw * mw / s);
13671  gamma = sqrt_sGeV/(2.0 * mw);
13672  gamma2= gamma*gamma;
13673 
13674 // J=1 Subamplitudes: Z
13675  gslpp::complex AZpp, AZmm, AZp0, AZm0, AZ0p, AZ0m, AZ00;
13676 
13677  AZpp = gslpp::complex(g1Z + 2.0* gamma2* lambdaZ, (ktZ + lambdatZ - 2.0*lambdatZ)/beta , false);
13678  AZmm = gslpp::complex(g1Z + 2.0* gamma2* lambdaZ, -(ktZ + lambdatZ - 2.0*lambdatZ)/beta , false);
13679  AZp0 = gslpp::complex(f3Z + beta * g5Z , -g4Z + (ktZ-lambdatZ)/beta , false);
13680  AZp0 = gamma * AZp0;
13681  AZm0 = gslpp::complex(f3Z - beta * g5Z , -g4Z - (ktZ-lambdatZ)/beta , false);
13682  AZm0 = gamma * AZm0;
13683  AZ0p = gslpp::complex(f3Z - beta * g5Z , g4Z + (ktZ-lambdatZ)/beta , false);
13684  AZ0p = gamma * AZ0p;
13685  AZ0m = gslpp::complex(f3Z + beta * g5Z , g4Z - (ktZ-lambdatZ)/beta , false);
13686  AZ0m = gamma * AZ0m;
13687  AZ00 = gslpp::complex( g1Z + 2.0*gamma2*kZ, 0.0 , false);
13688 
13689 // Collect in matrices and separate LH and RH
13690  gslpp::matrix<gslpp::complex> AmpZLH(3, 3, 0.0);
13691  gslpp::matrix<gslpp::complex> AmpZRH(3, 3, 0.0);
13692 
13693  AmpZLH.assign(0,0, AZpp * d1LH(0,0) );
13694  AmpZLH.assign(0,1, AZp0 * d1LH(0,1));
13695  AmpZLH.assign(0,2, 0.0);
13696 
13697  AmpZLH.assign(1,0, AZ0p * d1LH(1,0));
13698  AmpZLH.assign(1,1, AZ00 * d1LH(1,1));
13699  AmpZLH.assign(1,2, AZ0m * d1LH(1,2));
13700 
13701  AmpZLH.assign(2,0, 0.0);
13702  AmpZLH.assign(2,1, AZm0 * d1LH(2,1));
13703  AmpZLH.assign(2,2, AZmm * d1LH(2,2));
13704 
13705  AmpZLH = AmpZLH * beta * s/(s-Mz*Mz);
13706 
13707 // Add the correct Zff coupling
13708  AmpZLH = AmpZLH * gLe / sW2_tree;
13709 
13710  AmpZRH.assign(0,0, AZpp * d1RH(0,0) );
13711  AmpZRH.assign(0,1, AZp0 * d1RH(0,1));
13712  AmpZRH.assign(0,2, 0.0);
13713 
13714  AmpZRH.assign(1,0, AZ0p * d1RH(1,0));
13715  AmpZRH.assign(1,1, AZ00 * d1RH(1,1));
13716  AmpZRH.assign(1,2, AZ0m * d1RH(1,2));
13717 
13718  AmpZRH.assign(2,0, 0.0);
13719  AmpZRH.assign(2,1, AZm0 * d1RH(2,1));
13720  AmpZRH.assign(2,2, AZmm * d1RH(2,2));
13721 
13722  AmpZRH = AmpZRH * beta * s/(s-Mz*Mz);
13723 
13724 // Add the correct Zff coupling
13725  AmpZRH = AmpZRH * gRe / sW2_tree;
13726 
13727 // J=1 Subamplitudes: gamma
13728  gslpp::complex Agapp, Agamm, Agap0, Agam0, Aga0p, Aga0m, Aga00;
13729 
13730  Agapp = gslpp::complex(g1ga + 2.0* gamma2* lambdaga, (ktga + lambdatga - 2.0*lambdatga)/beta , false);
13731  Agamm = gslpp::complex(g1ga + 2.0* gamma2* lambdaga, -(ktga + lambdatga - 2.0*lambdatga)/beta , false);
13732  Agap0 = gslpp::complex(f3ga + beta * g5ga , -g4ga + (ktga-lambdatga)/beta , false);
13733  Agap0 = gamma * Agap0;
13734  Agam0 = gslpp::complex(f3ga - beta * g5ga , -g4ga - (ktga-lambdatga)/beta , false);
13735  Agam0 = gamma * Agam0;
13736  Aga0p = gslpp::complex(f3ga - beta * g5ga , g4ga + (ktga-lambdatga)/beta , false);
13737  Aga0p = gamma * Aga0p;
13738  Aga0m = gslpp::complex(f3ga + beta * g5ga , g4ga - (ktga-lambdatga)/beta , false);
13739  Aga0m = gamma * Aga0m;
13740  Aga00 = gslpp::complex( g1ga + 2.0*gamma2*kga, 0.0 , false);
13741 
13742 // Collect in matrices. Here LH = RH, except for the Wigner functions
13743  gslpp::matrix<gslpp::complex> AmpgaLH(3, 3, 0.0);
13744  gslpp::matrix<gslpp::complex> AmpgaRH(3, 3, 0.0);
13745 
13746  AmpgaLH.assign(0,0, Agapp * d1LH(0,0));
13747  AmpgaLH.assign(0,1, Agap0 * d1LH(0,1));
13748  AmpgaLH.assign(0,2, 0.0);
13749 
13750  AmpgaLH.assign(1,0, Aga0p * d1LH(1,0));
13751  AmpgaLH.assign(1,1, Aga00 * d1LH(1,1));
13752  AmpgaLH.assign(1,2, Aga0m * d1LH(1,2));
13753 
13754  AmpgaLH.assign(2,0, 0.0);
13755  AmpgaLH.assign(2,1, Agam0 * d1LH(2,1));
13756  AmpgaLH.assign(2,2, Agamm * d1LH(2,2));
13757 
13758  AmpgaRH.assign(0,0, Agapp * d1RH(0,0));
13759  AmpgaRH.assign(0,1, Agap0 * d1RH(0,1));
13760  AmpgaRH.assign(0,2, 0.0);
13761 
13762  AmpgaRH.assign(1,0, Aga0p * d1RH(1,0));
13763  AmpgaRH.assign(1,1, Aga00 * d1RH(1,1));
13764  AmpgaRH.assign(1,2, Aga0m * d1RH(1,2));
13765 
13766  AmpgaRH.assign(2,0, 0.0);
13767  AmpgaRH.assign(2,1, Agam0 * d1RH(2,1));
13768  AmpgaRH.assign(2,2, Agamm * d1RH(2,2));
13769 
13770  AmpgaLH = -beta * AmpgaLH;
13771  AmpgaRH = -beta * AmpgaRH;
13772 
13773 // J=1 Subamplitudes: neutrino
13774  gslpp::complex Bpp, Bmm, Bp0, Bm0, B0p, B0m, B00;
13775  gslpp::complex Cpp, Cmm, Cp0, Cm0, C0p, C0m, C00;
13776 
13777  Bpp = gslpp::complex(1.0 , 0.0 , false);
13778  Bmm = Bpp;
13779  Bp0 = gslpp::complex( 2.0 * gamma, 0.0 , false);
13780  Bm0 = Bp0;
13781  B0p = Bp0;
13782  B0m = Bp0;
13783  B00 = gslpp::complex( 2.0 * gamma2, 0.0 , false);
13784 
13785  Cpp = gslpp::complex(1.0/gamma2 , 0.0 , false);
13786  Cmm = Cpp;
13787  Cp0 = gslpp::complex( 2.0 * (1.0 + beta)/gamma, 0.0 , false);
13788  Cm0 = gslpp::complex( 2.0 * (1.0 - beta)/gamma, 0.0 , false);
13789  C0p = Cm0;
13790  C0m = Cp0;
13791  C00 = gslpp::complex( 2.0 / gamma2, 0.0 , false);
13792 
13793 // Collect in matrices. Here LH = RH
13794  gslpp::matrix<gslpp::complex> Bnu(3, 3, 0.0);
13795  gslpp::matrix<gslpp::complex> Cnu(3, 3, 0.0);
13796 
13797  Bnu.assign(0,0, Bpp * d1LH(0,0));
13798  Bnu.assign(0,1, Bp0 * d1LH(0,1));
13799  Bnu.assign(0,2, 0.0);
13800 
13801  Bnu.assign(1,0, B0p * d1LH(1,0));
13802  Bnu.assign(1,1, B00 * d1LH(1,1));
13803  Bnu.assign(1,2, B0m * d1LH(1,2));
13804 
13805  Bnu.assign(2,0, 0.0);
13806  Bnu.assign(2,1, Bm0 * d1LH(2,1));
13807  Bnu.assign(2,2, Bmm * d1LH(2,2));
13808 
13809  Cnu.assign(0,0, Cpp * d1LH(0,0));
13810  Cnu.assign(0,1, Cp0 * d1LH(0,1));
13811  Cnu.assign(0,2, 0.0);
13812 
13813  Cnu.assign(1,0, C0p * d1LH(1,0));
13814  Cnu.assign(1,1, C00 * d1LH(1,1));
13815  Cnu.assign(1,2, C0m * d1LH(1,2));
13816 
13817  Cnu.assign(2,0, 0.0);
13818  Cnu.assign(2,1, Cm0 * d1LH(2,1));
13819  Cnu.assign(2,2, Cmm * d1LH(2,2));
13820 
13821 // The matrix with the total J=1 neutrino amplitude (only LH neutrinos)
13822  gslpp::matrix<gslpp::complex> Ampnu1(3, 3, 0.0);
13823 
13824  Ampnu1 = Bnu - Cnu/(1.0 + beta*beta - 2.0 * beta * cos);
13825 
13826  Ampnu1 = Uenu * Uenu.conjugate() * Ampnu1 / (2.0 * beta * sW2_tree);
13827 
13828  gslpp::matrix<gslpp::complex> Ampnu2(3, 3, 0.0);
13829 
13830  Ampnu2.assign(0,2, (1.0 - cos)/2.0 );
13831  Ampnu2.assign(1,1, 0.0);
13832  Ampnu2.assign(2,0, -(1.0 + cos)/2.0);
13833 
13834  Ampnu2 = (8.0 * M_PI * aleMz / sW2_tree)* Uenu * Uenu.conjugate() * Ampnu2 * sin / (1.0 + beta*beta - 2.0*beta*cos);
13835 
13836 // Total amplitudes
13837  gslpp::matrix<gslpp::complex> MRH(3, 3, 0.0);
13838  gslpp::matrix<gslpp::complex> MLH(3, 3, 0.0);
13839 
13840  MRH = sqrt(2.0) * 4.0 * M_PI * aleMz * (AmpZRH + AmpgaRH);
13841  MLH = - sqrt(2.0) * 4.0 * M_PI * aleMz * (AmpZLH + AmpgaLH + Ampnu1) + Ampnu2;
13842 
13843 // Total amplitude squared and differential cross section (in pb)
13844  gslpp::matrix<double> M2(3, 3, 0.0);
13845  double dxsdcos;
13846 
13847  dxsdcos = 0.0;
13848 
13849  for (int i=0; i<3; i++) {
13850  for (int j=0; j<3; j++) {
13851  M2.assign(i,j, (MRH(i,j)* (MRH(i,j).conjugate())
13852  + MLH(i,j)* (MLH(i,j).conjugate())).real() );
13853 
13854  dxsdcos = dxsdcos + M2(i,j);
13855  }
13856  }
13857 
13858 // Differential cross section in pb
13859  dxsdcos = (topb * beta / 32.0 / M_PI / s) * dxsdcos;
13860 
13861  return dxsdcos;
13862 }

◆ dxseeWWdcosBin()

double NPSMEFTd6::dxseeWWdcosBin ( const double  sqrt_s,
const double  cos1,
const double  cos2 
) const
virtual

The integral of differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\) in a given bin of the \(W\) polar angle.

Returns
\(\int_{\cos{\theta_1}}^{\cos{\theta_2}} d\sigma/d\cos{\theta}\)

< Gsl integral variable

< Gsl integral variable

< Gsl integral variable

Reimplemented from NPbase.

Definition at line 13864 of file NPSMEFTd6.cpp.

13865 {
13866  double xsWWbin;
13867  double errWW;
13869  gsl_function FR;
13871  FR = convertToGslFunction(boost::bind(&NPSMEFTd6::dxseeWWdcos,&(*this), sqrt_s, _1));
13872 
13873  gsl_integration_cquad(&FR, cos1, cos2, 1.e-5, 1.e-4, w_WW, &xsWWbin, &errWW, NULL);
13874 
13875 // Simple integration for testing
13876 // double cosx;
13877 
13878 // xsWWbin = 0.0;
13879 
13880 // for (int i=1; i<100; i++){
13881 // cosx = cos1 + i*(cos2-cos1)/100;
13882 // xsWWbin = xsWWbin + dxseeWWdcos(sqrt_s, cosx);
13883 // }
13884 
13885 // xsWWbin = xsWWbin + 0.5 * (dxseeWWdcos(sqrt_s, cos1) + dxseeWWdcos(sqrt_s, cos2));
13886 
13887 // xsWWbin = xsWWbin * (cos2-cos1)/100;
13888 
13889 // Compute the BR into e nu, mu nu for one W and into jets for the other
13890  double BRlv, BRjj;
13891 
13892  BRlv = GammaW(leptons[NEUTRINO_1], leptons[ELECTRON]) +
13895 
13896  BRjj = GammaW() - BRlv;
13897 
13898  BRlv = BRlv - GammaW(leptons[NEUTRINO_3], leptons[TAU]);
13899 
13900  BRlv =BRlv / GammaW();
13901 
13902  BRjj =BRjj / GammaW();
13903 
13904 
13905 
13906  return xsWWbin * BRlv * BRjj;
13907 }

◆ f_triangle()

gslpp::complex NPSMEFTd6::f_triangle ( const double  tau) const

Loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings.

Parameters
[in]

Definition at line 3227 of file NPSMEFTd6.cpp.

3228 {
3229  gslpp::complex tmp;
3230  if (tau >= 1.0) {
3231  tmp = asin(1.0 / sqrt(tau));
3232  return (tmp * tmp);
3233  } else {
3234  tmp = log((1.0 + sqrt(1.0 - tau)) / (1.0 - sqrt(1.0 - tau))) - M_PI * gslpp::complex::i();
3235  return (-0.25 * tmp * tmp);
3236  }
3237 }

◆ g_triangle()

gslpp::complex NPSMEFTd6::g_triangle ( const double  tau) const

Loop function entering in the calculation of the effective \(HZ\gamma\) coupling.

Parameters
[in]

Definition at line 3239 of file NPSMEFTd6.cpp.

3240 {
3241  gslpp::complex tmp;
3242  if (tau >= 1.0) {
3243  tmp = sqrt(tau -1.0) * asin(1.0 / sqrt(tau));
3244  return tmp;
3245  } else {
3246  tmp = sqrt(1.0 - tau) * ( log((1.0 + sqrt(1.0 - tau)) / (1.0 - sqrt(1.0 - tau))) - M_PI * gslpp::complex::i() );
3247  return 0.5 * tmp;
3248  }
3249 }

◆ GammaHbbRatio()

double NPSMEFTd6::GammaHbbRatio ( ) const

The ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to bb)\)/ \(\Gamma(H\to bb)_{\mathrm{SM}}\)

Definition at line 12324 of file NPSMEFTd6.cpp.

12325 {
12326  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
12327  double width = 1.0;
12328 
12329  width += deltaGammaHbbRatio1();
12330 
12331  if (FlagQuadraticTerms) {
12332  //Add contributions that are quadratic in the effective coefficients
12333  width += deltaGammaHbbRatio2();
12334  }
12335 
12336  return width;
12337 }

◆ GammaHccRatio()

double NPSMEFTd6::GammaHccRatio ( ) const

The ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to cc)\)/ \(\Gamma(H\to cc)_{\mathrm{SM}}\)

Definition at line 12258 of file NPSMEFTd6.cpp.

12259 {
12260  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
12261  double width = 1.0;
12262 
12263  width += deltaGammaHccRatio1();
12264 
12265  if (FlagQuadraticTerms) {
12266  //Add contributions that are quadratic in the effective coefficients
12267  width += deltaGammaHccRatio2();
12268  }
12269 
12270  return width;
12271 
12272 }

◆ GammaHgagaRatio()

double NPSMEFTd6::GammaHgagaRatio ( ) const

The ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to \gamma\gamma)\)/ \(\Gamma(H\to \gamma\gamma)_{\mathrm{SM}}\)

Definition at line 12077 of file NPSMEFTd6.cpp.

12078 {
12079  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
12080  double width = 1.0;
12081 
12082  width += deltaGammaHgagaRatio1();
12083 
12084  if (FlagQuadraticTerms) {
12085  //Add contributions that are quadratic in the effective coefficients
12086  width += deltaGammaHgagaRatio2();
12087  }
12088 
12089  return width;
12090 
12091 }

◆ GammaHggRatio()

double NPSMEFTd6::GammaHggRatio ( ) const

The ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to gg)\)/ \(\Gamma(H\to gg)_{\mathrm{SM}}\)

Definition at line 10648 of file NPSMEFTd6.cpp.

10649 {
10650  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
10651  double width = 1.0;
10652 
10653  width += deltaGammaHggRatio1();
10654 
10655  if (FlagQuadraticTerms) {
10656  //Add contributions that are quadratic in the effective coefficients
10657  width += deltaGammaHggRatio2();
10658  }
10659 
10660  return width;
10661 
10662 }

◆ GammaHmumuRatio()

double NPSMEFTd6::GammaHmumuRatio ( ) const

The ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to \mu\mu)\)/ \(\Gamma(H\to \mu\mu)_{\mathrm{SM}}\)

Definition at line 12153 of file NPSMEFTd6.cpp.

12154 {
12155  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
12156  double width = 1.0;
12157 
12158  width += deltaGammaHmumuRatio1();
12159 
12160  if (FlagQuadraticTerms) {
12161  //Add contributions that are quadratic in the effective coefficients
12162  width += deltaGammaHmumuRatio2();
12163  }
12164 
12165  return width;
12166 
12167 }

◆ GammaHtautauRatio()

double NPSMEFTd6::GammaHtautauRatio ( ) const

The ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to \tau\tau)\)/ \(\Gamma(H\to \tau\tau)_{\mathrm{SM}}\)

Definition at line 12205 of file NPSMEFTd6.cpp.

12206 {
12207  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
12208  double width = 1.0;
12209 
12210  width += deltaGammaHtautauRatio1();
12211 
12212  if (FlagQuadraticTerms) {
12213  //Add contributions that are quadratic in the effective coefficients
12214  width += deltaGammaHtautauRatio2();
12215  }
12216 
12217  return width;
12218 
12219 }

◆ GammaHWffRatio()

double NPSMEFTd6::GammaHWffRatio ( ) const

The ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model.

Returns
\(\Gamma(H\to W f f)\)/ \(\Gamma(H\to W f f)_{\mathrm{SM}}\)

Definition at line 10990 of file NPSMEFTd6.cpp.

10991 {
10992  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
10993  double width = 1.0;
10994 
10995  width += deltaGammaHWffRatio1();
10996 
10997  if (FlagQuadraticTerms) {
10998  //Add contributions that are quadratic in the effective coefficients
10999  width += deltaGammaHWffRatio2();
11000  }
11001 
11002  return width;
11003 
11004 }

◆ GammaHWjjRatio()

double NPSMEFTd6::GammaHWjjRatio ( ) const

The ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to W j j)\)/ \(\Gamma(H\to W j j)_{\mathrm{SM}}\)

Definition at line 10874 of file NPSMEFTd6.cpp.

10875 {
10876  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
10877  double width = 1.0;
10878 
10879  width += deltaGammaHWjjRatio1();
10880 
10881  if (FlagQuadraticTerms) {
10882  //Add contributions that are quadratic in the effective coefficients
10883  width += deltaGammaHWjjRatio2();
10884  }
10885 
10886  return width;
10887 
10888 }

◆ GammaHWlvRatio()

double NPSMEFTd6::GammaHWlvRatio ( ) const

The ratio of the \(\Gamma(H\to W l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to Wl\nu)\)/ \(\Gamma(H\to Wl\nu)_{\mathrm{SM}}\)

Definition at line 10757 of file NPSMEFTd6.cpp.

10758 {
10759  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
10760  double width = 1.0;
10761 
10762  width += deltaGammaHWlvRatio1();
10763 
10764  if (FlagQuadraticTerms) {
10765  //Add contributions that are quadratic in the effective coefficients
10766  width += deltaGammaHWlvRatio2();
10767  }
10768 
10769  return width;
10770 
10771 }

◆ GammaHWW2l2vRatio()

double NPSMEFTd6::GammaHWW2l2vRatio ( ) const

The ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to WW^*\to l\nu l\nu)\)/ \(\Gamma(H\to WW^*\to l\nu l\nu)_{\mathrm{SM}}\)

Definition at line 10813 of file NPSMEFTd6.cpp.

10814 {
10815  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
10816  double width = 1.0;
10817 
10818  width += deltaGammaHWW2l2vRatio1();
10819 
10820  if (FlagQuadraticTerms) {
10821  //Add contributions that are quadratic in the effective coefficients
10822  width += deltaGammaHWW2l2vRatio2();
10823  }
10824 
10825  return width;
10826 
10827 }

◆ GammaHWW4fRatio()

double NPSMEFTd6::GammaHWW4fRatio ( ) const

The ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model.

Returns
\(\Gamma(H\to WW^*\to 4f)\)/ \(\Gamma(H\to WW^*\to 4f)_{\mathrm{SM}}\)

Definition at line 11047 of file NPSMEFTd6.cpp.

11048 {
11049  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11050  double width = 1.0;
11051 
11052  width += deltaGammaHWW4fRatio1();
11053 
11054  if (FlagQuadraticTerms) {
11055  //Add contributions that are quadratic in the effective coefficients
11056  width += deltaGammaHWW4fRatio2();
11057  }
11058 
11059  return width;
11060 
11061 }

◆ GammaHWW4jRatio()

double NPSMEFTd6::GammaHWW4jRatio ( ) const

The ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to WW^*\to 4j)\)/ \(\Gamma(H\to WW^*\to 4j)_{\mathrm{SM}}\)

Definition at line 10930 of file NPSMEFTd6.cpp.

10931 {
10932  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
10933  double width = 1.0;
10934 
10935  width += deltaGammaHWW4jRatio1();
10936 
10937  if (FlagQuadraticTerms) {
10938  //Add contributions that are quadratic in the effective coefficients
10939  width += deltaGammaHWW4jRatio2();
10940  }
10941 
10942  return width;
10943 
10944 }

◆ GammaHWWRatio()

double NPSMEFTd6::GammaHWWRatio ( ) const

The ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to WW)\)/ \(\Gamma(H\to WW)_{\mathrm{SM}}\)

Definition at line 10709 of file NPSMEFTd6.cpp.

10710 {
10711  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
10712  double width = 1.0;
10713 
10714  width += deltaGammaHWWRatio1();
10715 
10716  if (FlagQuadraticTerms) {
10717  //Add contributions that are quadratic in the effective coefficients
10718  width += deltaGammaHWWRatio2();
10719  }
10720 
10721  return width;
10722 
10723 }

◆ GammaHZddRatio()

double NPSMEFTd6::GammaHZddRatio ( ) const

The ratio of the \(\Gamma(H\to Zd d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to Zd d)\)/ \(\Gamma(H\to Zd d)_{\mathrm{SM}}\)

Definition at line 11784 of file NPSMEFTd6.cpp.

11785 {
11786  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11787  double width = 1.0;
11788 
11789  width += deltaGammaHZddRatio1();
11790 
11791  if (FlagQuadraticTerms) {
11792  //Add contributions that are quadratic in the effective coefficients
11793  width += deltaGammaHZddRatio2();
11794  }
11795 
11796  return width;
11797 
11798 }

◆ GammaHZeeRatio()

double NPSMEFTd6::GammaHZeeRatio ( ) const

The ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to Zee)\)/ \(\Gamma(H\to Zee)_{\mathrm{SM}}\)

Definition at line 11224 of file NPSMEFTd6.cpp.

11225 {
11226  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11227  double width = 1.0;
11228 
11229  width += deltaGammaHZeeRatio1();
11230 
11231  if (FlagQuadraticTerms) {
11232  //Add contributions that are quadratic in the effective coefficients
11233  width += deltaGammaHZeeRatio2();
11234  }
11235 
11236  return width;
11237 
11238 }

◆ GammaHZffRatio()

double NPSMEFTd6::GammaHZffRatio ( ) const

The ratio of the \(\Gamma(H\to Zff)\), with \(f\) any fermion, in the current model and in the Standard Model.

Returns
\(\Gamma(H\to Zff)\)/ \(\Gamma(H\to Zff)_{\mathrm{SM}}\)

Definition at line 11843 of file NPSMEFTd6.cpp.

11844 {
11845  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11846  double width = 1.0;
11847 
11848  width += deltaGammaHZffRatio1();
11849 
11850  if (FlagQuadraticTerms) {
11851  //Add contributions that are quadratic in the effective coefficients
11852  width += deltaGammaHZffRatio2();
11853  }
11854 
11855  return width;
11856 
11857 }

◆ GammaHZgaRatio()

double NPSMEFTd6::GammaHZgaRatio ( ) const

The ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to Z\gamma)\)/ \(\Gamma(H\to Z\gamma)_{\mathrm{SM}}\)

Definition at line 11992 of file NPSMEFTd6.cpp.

11993 {
11994  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11995  double width = 1.0;
11996 
11997  width += deltaGammaHZgaRatio1();
11998 
11999  if (FlagQuadraticTerms) {
12000  //Add contributions that are quadratic in the effective coefficients
12001  width += deltaGammaHZgaRatio2();
12002  }
12003 
12004  return width;
12005 
12006 }

◆ GammaHZllRatio()

double NPSMEFTd6::GammaHZllRatio ( ) const

The ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to Zll)\)/ \(\Gamma(H\to Zll)_{\mathrm{SM}}\)

Definition at line 11165 of file NPSMEFTd6.cpp.

11166 {
11167  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11168  double width = 1.0;
11169 
11170  width += deltaGammaHZllRatio1();
11171 
11172  if (FlagQuadraticTerms) {
11173  //Add contributions that are quadratic in the effective coefficients
11174  width += deltaGammaHZllRatio2();
11175  }
11176 
11177  return width;
11178 
11179 }

◆ GammaHZmumuRatio()

double NPSMEFTd6::GammaHZmumuRatio ( ) const

The ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to Z\mu\mu)\)/ \(\Gamma(H\to Z\mu\mu)_{\mathrm{SM}}\)

Definition at line 11285 of file NPSMEFTd6.cpp.

11286 {
11287  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11288  double width = 1.0;
11289 
11290  width += deltaGammaHZmumuRatio1();
11291 
11292  if (FlagQuadraticTerms) {
11293  //Add contributions that are quadratic in the effective coefficients
11294  width += deltaGammaHZmumuRatio2();
11295  }
11296 
11297  return width;
11298 
11299 }

◆ GammaHZuuRatio()

double NPSMEFTd6::GammaHZuuRatio ( ) const

The ratio of the \(\Gamma(H\to Zu u)\) ( \(u=u,c \)) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to Zu u)\)/ \(\Gamma(H\to Zu u)_{\mathrm{SM}}\)

Definition at line 11725 of file NPSMEFTd6.cpp.

11726 {
11727  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11728  double width = 1.0;
11729 
11730  width += deltaGammaHZuuRatio1();
11731 
11732  if (FlagQuadraticTerms) {
11733  //Add contributions that are quadratic in the effective coefficients
11734  width += deltaGammaHZuuRatio2();
11735  }
11736 
11737  return width;
11738 
11739 }

◆ GammaHZvvRatio()

double NPSMEFTd6::GammaHZvvRatio ( ) const

The ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to Z\nu\nu)\)/ \(\Gamma(H\to Z\nu\nu)_{\mathrm{SM}}\)

Definition at line 11604 of file NPSMEFTd6.cpp.

11605 {
11606  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11607  double width = 1.0;
11608 
11609  width += deltaGammaHZvvRatio1();
11610 
11611  if (FlagQuadraticTerms) {
11612  //Add contributions that are quadratic in the effective coefficients
11613  width += deltaGammaHZvvRatio2();
11614  }
11615 
11616  return width;
11617 
11618 }

◆ GammaHZZ2e2muRatio()

double NPSMEFTd6::GammaHZZ2e2muRatio ( ) const

The ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to ZZ* \to 2e2\mu)\)/ \(\Gamma(H\to ZZ* \to 2e2\mu)_{\mathrm{SM}}\)

Definition at line 11479 of file NPSMEFTd6.cpp.

11480 {
11481  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11482  double width = 1.0;
11483 
11484  width += deltaGammaHZZ2e2muRatio1();
11485 
11486  if (FlagQuadraticTerms) {
11487  //Add contributions that are quadratic in the effective coefficients
11488  width += deltaGammaHZZ2e2muRatio2();
11489  }
11490 
11491  return width;
11492 
11493 }

◆ GammaHZZ4dRatio()

double NPSMEFTd6::GammaHZZ4dRatio ( ) const
inline

The ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to ZZ* \to 4 d)\)/ \(\Gamma(H\to ZZ* \to 4 d)_{\mathrm{SM}}\)

Definition at line 2255 of file NPSMEFTd6.h.

2256  {
2257  return 1.0;
2258  };

◆ GammaHZZ4eRatio()

double NPSMEFTd6::GammaHZZ4eRatio ( ) const

The ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to ZZ* \to 4e)\)/ \(\Gamma(H\to ZZ* \to 4e)_{\mathrm{SM}}\)

Definition at line 11416 of file NPSMEFTd6.cpp.

11417 {
11418  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11419  double width = 1.0;
11420 
11421  width += deltaGammaHZZ4eRatio1();
11422 
11423  if (FlagQuadraticTerms) {
11424  //Add contributions that are quadratic in the effective coefficients
11425  width += deltaGammaHZZ4eRatio2();
11426  }
11427 
11428  return width;
11429 
11430 }

◆ GammaHZZ4fRatio()

double NPSMEFTd6::GammaHZZ4fRatio ( ) const

The ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model.

Returns
\(\Gamma(H\to ZZ* \to 4f)\)/ \(\Gamma(H\to ZZ* \to 4f)_{\mathrm{SM}}\)

Definition at line 11906 of file NPSMEFTd6.cpp.

11907 {
11908  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11909  double width = 1.0;
11910 
11911  width += deltaGammaHZZ4fRatio1();
11912 
11913  if (FlagQuadraticTerms) {
11914  //Add contributions that are quadratic in the effective coefficients
11915  width += deltaGammaHZZ4fRatio2();
11916  }
11917 
11918  return width;
11919 
11920 }

◆ GammaHZZ4lRatio()

double NPSMEFTd6::GammaHZZ4lRatio ( ) const

The ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to ZZ* \to 4l)\)/ \(\Gamma(H\to ZZ* \to 4l)_{\mathrm{SM}}\)

Definition at line 11346 of file NPSMEFTd6.cpp.

11347 {
11348  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11349  double width = 1.0;
11350 
11351  width += deltaGammaHZZ4lRatio1();
11352 
11353  if (FlagQuadraticTerms) {
11354  //Add contributions that are quadratic in the effective coefficients
11355  width += deltaGammaHZZ4lRatio2();
11356  }
11357 
11358  return width;
11359 
11360 }

◆ GammaHZZ4muRatio()

double NPSMEFTd6::GammaHZZ4muRatio ( ) const

The ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to ZZ* \to 4\mu)\)/ \(\Gamma(H\to ZZ* \to 4\mu)_{\mathrm{SM}}\)

Definition at line 11541 of file NPSMEFTd6.cpp.

11542 {
11543  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11544  double width = 1.0;
11545 
11546  width += deltaGammaHZZ4muRatio1();
11547 
11548  if (FlagQuadraticTerms) {
11549  //Add contributions that are quadratic in the effective coefficients
11550  width += deltaGammaHZZ4muRatio2();
11551  }
11552 
11553  return width;
11554 
11555 }

◆ GammaHZZ4uRatio()

double NPSMEFTd6::GammaHZZ4uRatio ( ) const
inline

The ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to ZZ* \to 4u)\)/ \(\Gamma(H\to ZZ* \to 4u)_{\mathrm{SM}}\)

Definition at line 2240 of file NPSMEFTd6.h.

2241  {
2242  return 1.0;
2243  };

◆ GammaHZZ4vRatio()

double NPSMEFTd6::GammaHZZ4vRatio ( ) const

The ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to ZZ* \to 4\nu)\)/ \(\Gamma(H\to ZZ* \to 4\nu)_{\mathrm{SM}}\)

Definition at line 11662 of file NPSMEFTd6.cpp.

11663 {
11664  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11665  double width = 1.0;
11666 
11667  width += deltaGammaHZZ4vRatio1();
11668 
11669  if (FlagQuadraticTerms) {
11670  //Add contributions that are quadratic in the effective coefficients
11671  width += deltaGammaHZZ4vRatio2();
11672  }
11673 
11674  return width;
11675 
11676 }

◆ GammaHZZRatio()

double NPSMEFTd6::GammaHZZRatio ( ) const

The ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to ZZ)\)/ \(\Gamma(H\to ZZ)_{\mathrm{SM}}\)

Definition at line 11117 of file NPSMEFTd6.cpp.

11118 {
11119  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11120  double width = 1.0;
11121 
11122  width += deltaGammaHZZRatio1();
11123 
11124  if (FlagQuadraticTerms) {
11125  //Add contributions that are quadratic in the effective coefficients
11126  width += deltaGammaHZZRatio2();
11127  }
11128 
11129  return width;
11130 
11131 }

◆ GammaW() [1/2]

double NPSMEFTd6::GammaW ( ) const
virtual

The total width of the \(W\) boson, \(\Gamma_W\).

Returns
\(\Gamma_W\) in GeV

Reimplemented from NPbase.

Definition at line 2813 of file NPSMEFTd6.cpp.

2814 {
2815  return ( trueSM.GammaW() + deltaGamma_W() );
2816 }

◆ GammaW() [2/2]

double NPSMEFTd6::GammaW ( const Particle  fi,
const Particle  fj 
) const
virtual

A partial decay width of the \(W\) boson decay into a SM fermion pair.

Parameters
[in]fia lepton or quark
[in]fja lepton or quark
Returns
\(\Gamma^W_{ij}\)

Reimplemented from NPbase.

Definition at line 2795 of file NPSMEFTd6.cpp.

2796 {
2797  return ( trueSM.GammaW(fi, fj) + deltaGamma_Wff(fi, fj) );
2798 }

◆ getCed_1123()

double NPSMEFTd6::getCed_1123 ( ) const
inline

Return NP coeff Ced_1123.

Returns
\( Ced_1123 \)

Definition at line 984 of file NPSMEFTd6.h.

984  {
985  return Ced_1123;
986  }

◆ getCed_2223()

double NPSMEFTd6::getCed_2223 ( ) const
inline

Return NP coeff Ced_2223.

Returns
\( Ced_2223 \)

Definition at line 992 of file NPSMEFTd6.h.

992  {
993  return Ced_2223;
994  }

◆ getCeu_1133()

double NPSMEFTd6::getCeu_1133 ( ) const
inline

Return NP coeff Ceu_1133.

Returns
\( Ceu_1133 \)

Definition at line 1048 of file NPSMEFTd6.h.

1048  {
1049  return Ceu_1133;
1050  }

◆ getCeu_2233()

double NPSMEFTd6::getCeu_2233 ( ) const
inline

Return NP coeff Ceu_2233.

Returns
\( Ceu_2233 \)

Definition at line 1056 of file NPSMEFTd6.h.

1056  {
1057  return Ceu_2233;
1058  }

◆ getCHe_11()

double NPSMEFTd6::getCHe_11 ( ) const
inline

Return NP coeff CHe_11.

Returns
\( CHe_11 \)

Definition at line 1032 of file NPSMEFTd6.h.

1032  {
1033  return CHe_11;
1034  }

◆ getCHe_22()

double NPSMEFTd6::getCHe_22 ( ) const
inline

Return NP coeff CHe_22.

Returns
\( CHe_22 \)

Definition at line 1040 of file NPSMEFTd6.h.

1040  {
1041  return CHe_22;
1042  }

◆ getCHL1_11()

double NPSMEFTd6::getCHL1_11 ( ) const
inline

Return NP coeff CHL1_11.

Returns
\( CHL1_11 \)

Definition at line 1000 of file NPSMEFTd6.h.

1000  {
1001  return CHL1_11;
1002  }

◆ getCHL1_22()

double NPSMEFTd6::getCHL1_22 ( ) const
inline

Return NP coeff CHL1_22.

Returns
\( CHL1_22 \)

Definition at line 1008 of file NPSMEFTd6.h.

1008  {
1009  return CHL1_22;
1010  }

◆ getCHL3_11()

double NPSMEFTd6::getCHL3_11 ( ) const
inline

Return NP coeff CHL3_11.

Returns
\( CHL3_11 \)

Definition at line 1016 of file NPSMEFTd6.h.

1016  {
1017  return CHL3_11;
1018  }

◆ getCHL3_22()

double NPSMEFTd6::getCHL3_22 ( ) const
inline

Return NP coeff CHL3_22.

Returns
\( CHL3_22 \)

Definition at line 1024 of file NPSMEFTd6.h.

1024  {
1025  return CHL3_22;
1026  }

◆ getCLd_1123()

double NPSMEFTd6::getCLd_1123 ( ) const
inline

Return NP coeff CLd_1123.

Returns
\( CLd_1123 \)

Definition at line 968 of file NPSMEFTd6.h.

968  {
969  return CLd_1123;
970  }

◆ getCLd_2223()

double NPSMEFTd6::getCLd_2223 ( ) const
inline

Return NP coeff CLd_2223.

Returns
\( CLd_2223 \)

Definition at line 976 of file NPSMEFTd6.h.

976  {
977  return CLd_2223;
978  }

◆ getCLedQ_11()

double NPSMEFTd6::getCLedQ_11 ( ) const
inline

Return NP coeff CLedq_11.

Returns
\( CLedq_11 \)

Definition at line 1080 of file NPSMEFTd6.h.

1080  {
1081  return CLedQ_11;
1082  }

◆ getCLedQ_22()

double NPSMEFTd6::getCLedQ_22 ( ) const
inline

Return NP coeff CLedq_22.

Returns
\( CLedq_22 \)

Definition at line 1088 of file NPSMEFTd6.h.

1088  {
1089  return CLedQ_22;
1090  }

◆ getCLQ1_1123()

double NPSMEFTd6::getCLQ1_1123 ( ) const
inline

Return NP coeff CLQ1_1123.

Returns
\( CLQ1_1123 \)

Definition at line 936 of file NPSMEFTd6.h.

936  {
937  return CLQ1_1123;
938  }

◆ getCLQ1_2223()

double NPSMEFTd6::getCLQ1_2223 ( ) const
inline

Return NP coeff CLQ1_2223.

Returns
\( CLQ1_2223 \)

Definition at line 944 of file NPSMEFTd6.h.

944  {
945  return CLQ1_2223;
946  }

◆ getCLQ3_1123()

double NPSMEFTd6::getCLQ3_1123 ( ) const
inline

Return NP coeff CLQ3_1123.

Returns
\( CLQ3_1123 \)

Definition at line 952 of file NPSMEFTd6.h.

952  {
953  return CLQ3_1123;
954  }

◆ getCLQ3_2223()

double NPSMEFTd6::getCLQ3_2223 ( ) const
inline

Return NP coeff CLQ3_2223.

Returns
\( CLQ3_2223 \)

Definition at line 960 of file NPSMEFTd6.h.

960  {
961  return CLQ3_2223;
962  }

◆ getCLu_1133()

double NPSMEFTd6::getCLu_1133 ( ) const
inline

Return NP coeff CLu_1133.

Returns
\( CLu_1133 \)

Definition at line 1064 of file NPSMEFTd6.h.

1064  {
1065  return CLu_1133;
1066  }

◆ getCLu_2233()

double NPSMEFTd6::getCLu_2233 ( ) const
inline

Return NP coeff CLu_2233.

Returns
\( CLu_2233 \)

Definition at line 1072 of file NPSMEFTd6.h.

1072  {
1073  return CLu_2233;
1074  }

◆ getCpLedQ_11()

double NPSMEFTd6::getCpLedQ_11 ( ) const
inline

Return NP coeff CpLedq_11.

Returns
\( CpLedq_11 \)

Definition at line 1096 of file NPSMEFTd6.h.

1096  {
1097  return CpLedQ_11;
1098  }

◆ getCpLedQ_22()

double NPSMEFTd6::getCpLedQ_22 ( ) const
inline

Return NP coeff CpLedq_22.

Returns
\( CpLedq \)

Definition at line 1104 of file NPSMEFTd6.h.

1104  {
1105  return CpLedQ_22;
1106  }

◆ getCQe_2311()

double NPSMEFTd6::getCQe_2311 ( ) const
inline

Return NP coeff CQe_2322.

Returns
\( CQe_2322 \)

Definition at line 920 of file NPSMEFTd6.h.

920  {
921  return CQe_2311;
922  }

◆ getCQe_2322()

double NPSMEFTd6::getCQe_2322 ( ) const
inline

Return NP coeff CQe_2322.

Returns
\( CQe_2311 \)

Definition at line 928 of file NPSMEFTd6.h.

928  {
929  return CQe_2322;
930  }

◆ getLambda_NP()

double NPSMEFTd6::getLambda_NP ( ) const
inline

Return Lambda_NP.

Returns
\( Lambda_NP \)

Definition at line 912 of file NPSMEFTd6.h.

912  {
913  return Lambda_NP;
914  }

◆ getMatching()

virtual NPSMEFTd6Matching& NPSMEFTd6::getMatching ( ) const
inlinevirtual

A method to get the Matching object for this model.

Returns
The matching object for this model

Reimplemented from StandardModel.

Definition at line 901 of file NPSMEFTd6.h.

902  {
903  return NPSMEFTd6M.getObj();
904  }

◆ I_triangle_1()

gslpp::complex NPSMEFTd6::I_triangle_1 ( const double  tau,
const double  lambda 
) const

Loop function entering in the calculation of the effective \(HZ\gamma\) coupling.

Parameters
[in]

Definition at line 3251 of file NPSMEFTd6.cpp.

3252 {
3253  gslpp::complex tmp;
3254 
3255  tmp = ( tau*lambda * (f_triangle(tau)- f_triangle(lambda)) + 2.0 * tau * (g_triangle(tau)- g_triangle(lambda)) ) / (tau-lambda);
3256 
3257  tmp = tau*lambda * ( 1.0 + tmp ) / (2.0*(tau-lambda));
3258 
3259  return tmp;
3260 }

◆ I_triangle_2()

gslpp::complex NPSMEFTd6::I_triangle_2 ( const double  tau,
const double  lambda 
) const

Loop function entering in the calculation of the effective \(HZ\gamma\) coupling.

Parameters
[in]

Definition at line 3262 of file NPSMEFTd6.cpp.

3263 {
3264  gslpp::complex tmp;
3265 
3266  tmp = - 0.5 * tau*lambda * (f_triangle(tau)- f_triangle(lambda)) / (tau-lambda);
3267 
3268  return tmp;
3269 }

◆ kappaAeff()

double NPSMEFTd6::kappaAeff ( ) const
virtual

The effective coupling \(\kappa_{A,eff}=\sqrt{\Gamma_{HAA}/\Gamma_{HAA}^{SM}}\).

Returns
\(\kappa_{A,eff}\)

Reimplemented from NPbase.

Definition at line 15131 of file NPSMEFTd6.cpp.

15132 {
15133  return sqrt(GammaHgagaRatio());
15134 }

◆ kappabeff()

double NPSMEFTd6::kappabeff ( ) const
virtual

The effective coupling \(\kappa_{b,eff}=\sqrt{\Gamma_{Hbb}/\Gamma_{Hbb}^{SM}}\).

Returns
\(\kappa_{b,eff}\)

Reimplemented from NPbase.

Definition at line 15111 of file NPSMEFTd6.cpp.

15112 {
15113  return sqrt(GammaHbbRatio());
15114 }

◆ kappaceff()

double NPSMEFTd6::kappaceff ( ) const
virtual

The effective coupling \(\kappa_{c,eff}=\sqrt{\Gamma_{Hcc}/\Gamma_{Hcc}^{SM}}\).

Returns
\(\kappa_{c,eff}\)

Reimplemented from NPbase.

Definition at line 15106 of file NPSMEFTd6.cpp.

15107 {
15108  return sqrt(GammaHccRatio());
15109 }

◆ kappaGeff()

double NPSMEFTd6::kappaGeff ( ) const
virtual

The effective coupling \(\kappa_{G,eff}=\sqrt{\Gamma_{HGG}/\Gamma_{HGG}^{SM}}\).

Returns
\(\kappa_{G,eff}\)

Reimplemented from NPbase.

Definition at line 15116 of file NPSMEFTd6.cpp.

15117 {
15118  return sqrt(GammaHggRatio());
15119 }

◆ kappamueff()

double NPSMEFTd6::kappamueff ( ) const
virtual

The effective coupling \(\kappa_{\mu,eff}=\sqrt{\Gamma_{H\mu\mu}/\Gamma_{H\mu\mu}^{SM}}\).

Returns
\(\kappa_{\mu,eff}\)

Reimplemented from NPbase.

Definition at line 15096 of file NPSMEFTd6.cpp.

15097 {
15098  return sqrt(GammaHmumuRatio());
15099 }

◆ kappataueff()

double NPSMEFTd6::kappataueff ( ) const
virtual

The effective coupling \(\kappa_{\tau,eff}=\sqrt{\Gamma_{H\tau\tau}/\Gamma_{H\tau\tau}^{SM}}\).

Returns
\(\kappa_{\tau,eff}\)

Reimplemented from NPbase.

Definition at line 15101 of file NPSMEFTd6.cpp.

15102 {
15103  return sqrt(GammaHtautauRatio());
15104 }

◆ kappaWeff()

double NPSMEFTd6::kappaWeff ( ) const
virtual

The effective coupling \(\kappa_{W,eff}=\sqrt{\Gamma_{HWW}/\Gamma_{HWW}^{SM}}\).

Returns
\(\kappa_{W,eff}\)

Reimplemented from NPbase.

Definition at line 15126 of file NPSMEFTd6.cpp.

15127 {
15128  return sqrt(GammaHWWRatio());
15129 }

◆ kappaZAeff()

double NPSMEFTd6::kappaZAeff ( ) const
virtual

The effective coupling \(\kappa_{ZA,eff}=\sqrt{\Gamma_{HZA}/\Gamma_{HZA}^{SM}}\).

Returns
\(\kappa_{ZA,eff}\)

Reimplemented from NPbase.

Definition at line 15136 of file NPSMEFTd6.cpp.

15137 {
15138  return sqrt(GammaHZgaRatio());
15139 }

◆ kappaZeff()

double NPSMEFTd6::kappaZeff ( ) const
virtual

The effective coupling \(\kappa_{Z,eff}=\sqrt{\Gamma_{HZZ}/\Gamma_{HZZ}^{SM}}\).

Returns
\(\kappa_{Z,eff}\)

Reimplemented from NPbase.

Definition at line 15121 of file NPSMEFTd6.cpp.

15122 {
15123  return sqrt(GammaHZZRatio());
15124 }

◆ lambdaZNP()

double NPSMEFTd6::lambdaZNP ( ) const
virtual

The new physics contribution to the anomalous triple gauge coupling \(\lambda_{Z}\).

Returns
\(\lambda_{Z}\)

Reimplemented from NPbase.

Definition at line 13526 of file NPSMEFTd6.cpp.

13527 {
13528  double NPdirect;
13529 
13530  /* Translate from LHCHXWG-INT-2015-001: Checked with own calculations */
13531  NPdirect = - (3.0 / 2.0) * (sqrt( 4.0 * M_PI * aleMz ) / sW_tree) * CiW * v2_over_LambdaNP2;
13532 
13533  return NPdirect + lambZ ;
13534 }

◆ lambz_HB()

double NPSMEFTd6::lambz_HB ( ) const
virtual

The Higgs-basis coupling \(\lambda_{z}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(\lambda_{z}\)

Reimplemented from NPbase.

Definition at line 15284 of file NPSMEFTd6.cpp.

15285 {
15286  double ciHB;
15287 
15288  ciHB = -(3.0/2.0)*(eeMz/sW_tree)*CiW*v2_over_LambdaNP2;
15289 
15290  return ciHB;
15291 }

◆ mueeHvv()

double NPSMEFTd6::mueeHvv ( const double  sqrt_s) const
virtual

The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{e^+e^- \to H\nu\bar{\nu}}\)

Reimplemented from NPbase.

Definition at line 3996 of file NPSMEFTd6.cpp.

3997 {
3998  double mu = 1.0;
3999 
4000  double C1 = 0.0;
4001 
4002 // For the Higgs trilinear dependence assume the WBF mechanism dominates
4003 
4004  if (sqrt_s == 0.240) {
4005 
4006  C1 = 0.0064;
4007 
4008  mu +=
4009  +121539. * CiHbox / LambdaNP2
4010  +328845. * CiHL1_11 / LambdaNP2
4011  -37798.9 * CiHe_11 / LambdaNP2
4012  +279733. * CiHL3_11 / LambdaNP2
4013  -196039. * CiHD / LambdaNP2
4014  -70718.5 * CiHB / LambdaNP2
4015  +29671.9 * CiHW / LambdaNP2
4016  -401378. * CiHWB / LambdaNP2
4017  -23969.3 * CiDHB / LambdaNP2
4018  -1814.47 * CiDHW / LambdaNP2
4019  -4.698 * DeltaGF()
4020  -5.463 * deltaMwd6()
4021  ;
4022 
4023  // Add modifications due to small variations of the SM parameters
4024  mu += cHSM * (
4025  +4.842 * deltaMz()
4026  -2.535 * deltaMh()
4027  -0.528 * deltaaMZ()
4028  +3.46 * deltaGmu() );
4029 
4030  if (FlagQuadraticTerms) {
4031  //Add contributions that are quadratic in the effective coefficients
4032  mu += 0.0;
4033  }
4034 
4035  } else if (sqrt_s == 0.250) {
4036 
4037  C1 = 0.0064;
4038 
4039  mu +=
4040  +120627. * CiHbox / LambdaNP2
4041  +256825. * CiHL1_11 / LambdaNP2
4042  -38677.5 * CiHe_11 / LambdaNP2
4043  +175735. * CiHL3_11 / LambdaNP2
4044  -201059. * CiHD / LambdaNP2
4045  -57405. * CiHB / LambdaNP2
4046  -9860.82 * CiHW / LambdaNP2
4047  -403474. * CiHWB / LambdaNP2
4048  -20447.1 * CiDHB / LambdaNP2
4049  -9672.74 * CiDHW / LambdaNP2
4050  -4.656 * DeltaGF()
4051  -5.633 * deltaMwd6()
4052  ;
4053 
4054  // Add modifications due to small variations of the SM parameters
4055  mu += cHSM * (
4056  +4.194 * deltaMz()
4057  -2.783 * deltaMh()
4058  -0.477 * deltaaMZ()
4059  +3.414 * deltaGmu() );
4060 
4061  if (FlagQuadraticTerms) {
4062  //Add contributions that are quadratic in the effective coefficients
4063  mu += 0.0;
4064  }
4065 
4066  } else if (sqrt_s == 0.350) {
4067 
4068  C1 = 0.0062;
4069 
4070  mu +=
4071  +120666. * CiHbox / LambdaNP2
4072  -19184.6 * CiHL1_11 / LambdaNP2
4073  -27432.1 * CiHe_11 / LambdaNP2
4074  -238244. * CiHL3_11 / LambdaNP2
4075  -204898. * CiHD / LambdaNP2
4076  +11833.5 * CiHB / LambdaNP2
4077  -94273.3 * CiHW / LambdaNP2
4078  -377703. * CiHWB / LambdaNP2
4079  +1111.63 * CiDHB / LambdaNP2
4080  -31735.2 * CiDHW / LambdaNP2
4081  -4.669 * DeltaGF()
4082  -5.329 * deltaMwd6()
4083  ;
4084 
4085  // Add modifications due to small variations of the SM parameters
4086  mu += cHSM * (
4087  +3.738 * deltaMz()
4088  -1.994 * deltaMh()
4089  -0.537 * deltaaMZ()
4090  +3.484 * deltaGmu() );
4091 
4092  if (FlagQuadraticTerms) {
4093  //Add contributions that are quadratic in the effective coefficients
4094  mu += 0.0;
4095  }
4096 
4097  } else if (sqrt_s == 0.365) {
4098 
4099  C1 = 0.0062; // Use the same as 350 GeV
4100 
4101  mu +=
4102  +120864. * CiHbox / LambdaNP2
4103  -24430. * CiHL1_11 / LambdaNP2
4104  -24398.7 * CiHe_11 / LambdaNP2
4105  -253414. * CiHL3_11 / LambdaNP2
4106  -204817. * CiHD / LambdaNP2
4107  +12826.5 * CiHB / LambdaNP2
4108  -93455. * CiHW / LambdaNP2
4109  -377489. * CiHWB / LambdaNP2
4110  +1693.48 * CiDHB / LambdaNP2
4111  -32834.7 * CiDHW / LambdaNP2
4112  -4.68 * DeltaGF()
4113  -5.265 * deltaMwd6()
4114  ;
4115 
4116  // Add modifications due to small variations of the SM parameters
4117  mu += cHSM * (
4118  +3.834 * deltaMz()
4119  -1.867 * deltaMh()
4120  -0.556 * deltaaMZ()
4121  +3.512 * deltaGmu() );
4122 
4123  if (FlagQuadraticTerms) {
4124  //Add contributions that are quadratic in the effective coefficients
4125  mu += 0.0;
4126  }
4127 
4128  } else if (sqrt_s == 0.380) {
4129 
4130  C1 = 0.0062; // Use the same as 350 GeV
4131 
4132  mu +=
4133  +120775. * CiHbox / LambdaNP2
4134  -27548.7 * CiHL1_11 / LambdaNP2
4135  -22022.3 * CiHe_11 / LambdaNP2
4136  -266603. * CiHL3_11 / LambdaNP2
4137  -204782. * CiHD / LambdaNP2
4138  +13052.3 * CiHB / LambdaNP2
4139  -92560.2 * CiHW / LambdaNP2
4140  -377461. * CiHWB / LambdaNP2
4141  +1916.19 * CiDHB / LambdaNP2
4142  -33824.9 * CiDHW / LambdaNP2
4143  -4.684 * DeltaGF()
4144  -5.221 * deltaMwd6()
4145  ;
4146 
4147  // Add modifications due to small variations of the SM parameters
4148  mu += cHSM * (
4149  +3.931 * deltaMz()
4150  -1.75 * deltaMh()
4151  -0.574 * deltaaMZ()
4152  +3.532 * deltaGmu() );
4153 
4154  if (FlagQuadraticTerms) {
4155  //Add contributions that are quadratic in the effective coefficients
4156  mu += 0.0;
4157  }
4158 
4159  } else if (sqrt_s == 0.500) {
4160 
4161  C1 = 0.0061;
4162 
4163  mu +=
4164  +120683. * CiHbox / LambdaNP2
4165  -26906.2 * CiHL1_11 / LambdaNP2
4166  -11055.8 * CiHe_11 / LambdaNP2
4167  -326940. * CiHL3_11 / LambdaNP2
4168  -204335. * CiHD / LambdaNP2
4169  +10505.8 * CiHB / LambdaNP2
4170  -82453.1 * CiHW / LambdaNP2
4171  -378407. * CiHWB / LambdaNP2
4172  +1889.64 * CiDHB / LambdaNP2
4173  -41332.3 * CiDHW / LambdaNP2
4174  -4.705 * DeltaGF()
4175  -4.943 * deltaMwd6()
4176  ;
4177 
4178  // Add modifications due to small variations of the SM parameters
4179  mu += cHSM * (
4180  +4.412 * deltaMz()
4181  -1.191 * deltaMh()
4182  -0.659 * deltaaMZ()
4183  +3.633 * deltaGmu() );
4184 
4185  if (FlagQuadraticTerms) {
4186  //Add contributions that are quadratic in the effective coefficients
4187  mu += 0.0;
4188  }
4189 
4190  } else if (sqrt_s == 1.0) {
4191 
4192  C1 = 0.0059;
4193 
4194  mu +=
4195  +120462. * CiHbox / LambdaNP2
4196  -9025.99 * CiHL1_11 / LambdaNP2
4197  -3124.38 * CiHe_11 / LambdaNP2
4198  -454282. * CiHL3_11 / LambdaNP2
4199  -204077. * CiHD / LambdaNP2
4200  +3421.94 * CiHB / LambdaNP2
4201  -61892.5 * CiHW / LambdaNP2
4202  -379786. * CiHWB / LambdaNP2
4203  +396.747 * CiDHB / LambdaNP2
4204  -63826.6 * CiDHW / LambdaNP2
4205  -4.711 * DeltaGF()
4206  -4.587 * deltaMwd6()
4207  ;
4208 
4209  // Add modifications due to small variations of the SM parameters
4210  mu += cHSM * (
4211  +4.969 * deltaMz()
4212  -0.583 * deltaMh()
4213  -0.745 * deltaaMZ()
4214  +3.729 * deltaGmu() );
4215 
4216  if (FlagQuadraticTerms) {
4217  //Add contributions that are quadratic in the effective coefficients
4218  mu += 0.0;
4219  }
4220 
4221  } else if (sqrt_s == 1.4) {
4222 
4223  C1 = 0.0058;
4224 
4225  mu +=
4226  +120512. * CiHbox / LambdaNP2
4227  -4746.27 * CiHL1_11 / LambdaNP2
4228  -2212.55 * CiHe_11 / LambdaNP2
4229  -521829. * CiHL3_11 / LambdaNP2
4230  -204054. * CiHD / LambdaNP2
4231  +1891.37 * CiHB / LambdaNP2
4232  -54492.9 * CiHW / LambdaNP2
4233  -379916. * CiHWB / LambdaNP2
4234  +142.745 * CiDHB / LambdaNP2
4235  -75976. * CiDHW / LambdaNP2
4236  -4.712 * DeltaGF()
4237  -4.486 * deltaMwd6()
4238  ;
4239 
4240  // Add modifications due to small variations of the SM parameters
4241  mu += cHSM * (
4242  +5.108 * deltaMz()
4243  -0.447 * deltaMh()
4244  -0.767 * deltaaMZ()
4245  +3.751 * deltaGmu() );
4246 
4247  if (FlagQuadraticTerms) {
4248  //Add contributions that are quadratic in the effective coefficients
4249  mu += 0.0;
4250  }
4251 
4252  } else if (sqrt_s == 1.5) {
4253 
4254  C1 = 0.0058;// Use the same as 1400 GeV
4255 
4256  mu +=
4257  +120512. * CiHbox / LambdaNP2
4258  -4105.67 * CiHL1_11 / LambdaNP2
4259  -2086.49 * CiHe_11 / LambdaNP2
4260  -536150. * CiHL3_11 / LambdaNP2
4261  -204072. * CiHD / LambdaNP2
4262  +1682.65 * CiHB / LambdaNP2
4263  -53138.1 * CiHW / LambdaNP2
4264  -379943. * CiHWB / LambdaNP2
4265  +134.612 * CiDHB / LambdaNP2
4266  -78546.2 * CiDHW / LambdaNP2
4267  -4.711 * DeltaGF()
4268  -4.469 * deltaMwd6()
4269  ;
4270 
4271  // Add modifications due to small variations of the SM parameters
4272  mu += cHSM * (
4273  +5.132 * deltaMz()
4274  -0.424 * deltaMh()
4275  -0.773 * deltaaMZ()
4276  +3.757 * deltaGmu() );
4277 
4278  if (FlagQuadraticTerms) {
4279  //Add contributions that are quadratic in the effective coefficients
4280  mu += 0.0;
4281  }
4282 
4283  } else if (sqrt_s == 3.0) {
4284 
4285  C1 = 0.0057;
4286 
4287  mu +=
4288  +120404. * CiHbox / LambdaNP2
4289  -1215.14 * CiHL1_11 / LambdaNP2
4290  -1382.75 * CiHe_11 / LambdaNP2
4291  -686451. * CiHL3_11 / LambdaNP2
4292  -204039. * CiHD / LambdaNP2
4293  +293.31 * CiHB / LambdaNP2
4294  -41440.6 * CiHW / LambdaNP2
4295  -380130. * CiHWB / LambdaNP2
4296  -272.36 * CiDHB / LambdaNP2
4297  -104900. * CiDHW / LambdaNP2
4298  -4.706 * DeltaGF()
4299  -4.343 * deltaMwd6()
4300  ;
4301 
4302  // Add modifications due to small variations of the SM parameters
4303  mu += cHSM * (
4304  +5.307 * deltaMz()
4305  -0.283 * deltaMh()
4306  -0.802 * deltaaMZ()
4307  +3.789 * deltaGmu() );
4308 
4309  if (FlagQuadraticTerms) {
4310  //Add contributions that are quadratic in the effective coefficients
4311  mu += 0.0;
4312  }
4313 
4314  } else
4315  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvv()");
4316 
4317  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
4318  mu += eeeWBFint + eeeWBFpar;
4319 
4320 // Linear contribution from Higgs self-coupling
4321  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
4322 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
4324 
4325  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
4326 
4327  return mu;
4328 }

◆ mueeHvvPol()

double NPSMEFTd6::mueeHvvPol ( const double  sqrt_s,
const double  Pol_em,
const double  Pol_ep 
) const
virtual

The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively
Returns
\(\mu_{e^+e^- \to H\nu\bar{\nu}}\)

Reimplemented from NPbase.

Definition at line 4331 of file NPSMEFTd6.cpp.

4332 {
4333  double mu = 1.0;
4334 
4335  double C1 = 0.0;
4336 
4337 // For the Higgs trilinear dependence assume the WBF mechanism dominates
4338 
4339  if (sqrt_s == 0.240) {
4340 
4341  C1 = 0.0064;
4342 
4343  if (Pol_em == 80. && Pol_ep == -30.){
4344  mu +=
4345  +121180. * CiHbox / LambdaNP2
4346  +221479. * CiHL1_11 / LambdaNP2
4347  -508958. * CiHe_11 / LambdaNP2
4348  +220003. * CiHL3_11 / LambdaNP2
4349  -149238. * CiHD / LambdaNP2
4350  +24268.3 * CiHB / LambdaNP2
4351  -32411.5 * CiHW / LambdaNP2
4352  -194663. * CiHWB / LambdaNP2
4353  +29267.1 * CiDHB / LambdaNP2
4354  -11610.1 * CiDHW / LambdaNP2
4355  -3.633 * DeltaGF()
4356  -4.394 * deltaMwd6()
4357  ;
4358 
4359  // Add modifications due to small variations of the SM parameters
4360  mu += cHSM * ( +2.975 * deltaMz()
4361  -2.624 * deltaMh()
4362  +0.379 * deltaaMZ()
4363  +2.282 * deltaGmu() );
4364 
4365  } else if (Pol_em == -80. && Pol_ep == 30.){
4366  mu +=
4367  +121456. * CiHbox / LambdaNP2
4368  +337881. * CiHL1_11 / LambdaNP2
4369  +931.718 * CiHe_11 / LambdaNP2
4370  +283908. * CiHL3_11 / LambdaNP2
4371  -199920. * CiHD / LambdaNP2
4372  -78796.8 * CiHB / LambdaNP2
4373  +34606.7 * CiHW / LambdaNP2
4374  -418335. * CiHWB / LambdaNP2
4375  -28484. * CiDHB / LambdaNP2
4376  -1197.92 * CiDHW / LambdaNP2
4377  -4.781 * DeltaGF()
4378  -5.537 * deltaMwd6()
4379  ;
4380 
4381  // Add modifications due to small variations of the SM parameters
4382  mu += cHSM * ( +5.005 * deltaMz()
4383  -2.529 * deltaMh()
4384  -0.603 * deltaaMZ()
4385  +3.57 * deltaGmu() );
4386 
4387  } else if (Pol_em == 80. && Pol_ep == 0.){
4388  mu +=
4389  +121483. * CiHbox / LambdaNP2
4390  +266382. * CiHL1_11 / LambdaNP2
4391  -313151. * CiHe_11 / LambdaNP2
4392  +245682. * CiHL3_11 / LambdaNP2
4393  -168446. * CiHD / LambdaNP2
4394  -15072.1 * CiHB / LambdaNP2
4395  -6209.98 * CiHW / LambdaNP2
4396  -281195. * CiHWB / LambdaNP2
4397  +6468.72 * CiDHB / LambdaNP2
4398  -7633.09 * CiDHW / LambdaNP2
4399  -4.079 * DeltaGF()
4400  -4.832 * deltaMwd6()
4401  ;
4402 
4403  // Add modifications due to small variations of the SM parameters
4404  mu += cHSM * ( +3.758 * deltaMz()
4405  -2.579 * deltaMh()
4406  +0.009 * deltaaMZ()
4407  +2.778 * deltaGmu() );
4408 
4409  } else if (Pol_em == -80. && Pol_ep == 0.){
4410  mu +=
4411  +121500. * CiHbox / LambdaNP2
4412  +337280. * CiHL1_11 / LambdaNP2
4413  -1209.82 * CiHe_11 / LambdaNP2
4414  +283754. * CiHL3_11 / LambdaNP2
4415  -199723. * CiHD / LambdaNP2
4416  -78465.3 * CiHB / LambdaNP2
4417  +34393.4 * CiHW / LambdaNP2
4418  -417413. * CiHWB / LambdaNP2
4419  -28344.3 * CiDHB / LambdaNP2
4420  -1296.23 * CiDHW / LambdaNP2
4421  -4.777 * DeltaGF()
4422  -5.539 * deltaMwd6()
4423  ;
4424 
4425  // Add modifications due to small variations of the SM parameters
4426  mu += cHSM * ( +4.99 * deltaMz()
4427  -2.528 * deltaMh()
4428  -0.6 * deltaaMZ()
4429  +3.56 * deltaGmu() );
4430 
4431  } else {
4432  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
4433  }
4434 
4435  } else if (sqrt_s == 0.250) {
4436 
4437  C1 = 0.0064;
4438 
4439  if (Pol_em == 80. && Pol_ep == -30.){
4440  mu +=
4441  +120626. * CiHbox / LambdaNP2
4442  +172936. * CiHL1_11 / LambdaNP2
4443  -516799. * CiHe_11 / LambdaNP2
4444  +146366. * CiHL3_11 / LambdaNP2
4445  -156275. * CiHD / LambdaNP2
4446  +30993.1 * CiHB / LambdaNP2
4447  -62277.2 * CiHW / LambdaNP2
4448  -213096. * CiHWB / LambdaNP2
4449  +32593.7 * CiDHB / LambdaNP2
4450  -18479.4 * CiDHW / LambdaNP2
4451  -3.678 * DeltaGF()
4452  -4.598 * deltaMwd6()
4453  ;
4454 
4455  // Add modifications due to small variations of the SM parameters
4456  mu += cHSM * ( +2.739 * deltaMz()
4457  -2.661 * deltaMh()
4458  +0.356 * deltaaMZ()
4459  +2.343 * deltaGmu() );
4460 
4461  } else if (Pol_em == -80. && Pol_ep == 30.){
4462  mu +=
4463  +120567. * CiHbox / LambdaNP2
4464  +263666. * CiHL1_11 / LambdaNP2
4465  -351.165 * CiHe_11 / LambdaNP2
4466  -396055. * CiHL3_11 / LambdaNP2
4467  -204612. * CiHD / LambdaNP2
4468  -64672.8 * CiHB / LambdaNP2
4469  -5618.64 * CiHW / LambdaNP2
4470  -418629. * CiHWB / LambdaNP2
4471  -24815.6 * CiDHB / LambdaNP2
4472  -9013.23 * CiDHW / LambdaNP2
4473  +286902. * CiLL_1221 / LambdaNP2
4474  -5.706 * deltaMwd6()
4475  ;
4476 
4477  // Add modifications due to small variations of the SM parameters
4478  mu += cHSM * ( +4.313 * deltaMz()
4479  -2.793 * deltaMh()
4480  -0.544 * deltaaMZ()
4481  +3.494 * deltaGmu() );
4482 
4483  } else if (Pol_em == 80. && Pol_ep == 0.){
4484  mu +=
4485  +120240. * CiHbox / LambdaNP2
4486  +208124. * CiHL1_11 / LambdaNP2
4487  -315248. * CiHe_11 / LambdaNP2
4488  +158895. * CiHL3_11 / LambdaNP2
4489  -175074. * CiHD / LambdaNP2
4490  -6529.15 * CiHB / LambdaNP2
4491  -40099.4 * CiHW / LambdaNP2
4492  -293696. * CiHWB / LambdaNP2
4493  +10284.9 * CiDHB / LambdaNP2
4494  -15311.7 * CiDHW / LambdaNP2
4495  -4.092 * DeltaGF()
4496  -5.01 * deltaMwd6()
4497  ;
4498 
4499  // Add modifications due to small variations of the SM parameters
4500  mu += cHSM * ( +3.351 * deltaMz()
4501  -2.698 * deltaMh()
4502  -0.006 * deltaaMZ()
4503  +2.791 * deltaGmu() );
4504 
4505  } else if (Pol_em == -80. && Pol_ep == 0.){
4506  mu +=
4507  +120459. * CiHbox / LambdaNP2
4508  +263262. * CiHL1_11 / LambdaNP2
4509  -2507.98 * CiHe_11 / LambdaNP2
4510  +177390. * CiHL3_11 / LambdaNP2
4511  -204514. * CiHD / LambdaNP2
4512  -64371.5 * CiHB / LambdaNP2
4513  -5927.95 * CiHW / LambdaNP2
4514  -417860. * CiHWB / LambdaNP2
4515  -24699.8 * CiDHB / LambdaNP2
4516  -9119.93 * CiDHW / LambdaNP2
4517  -4.726 * DeltaGF()
4518  -5.715 * deltaMwd6()
4519  ;
4520 
4521  // Add modifications due to small variations of the SM parameters
4522  mu += cHSM * ( +4.305 * deltaMz()
4523  -2.793 * deltaMh()
4524  -0.54 * deltaaMZ()
4525  +3.492 * deltaGmu() );
4526 
4527  } else {
4528  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
4529  }
4530 
4531  } else if (sqrt_s == 0.350) {
4532 
4533  C1 = 0.0062;
4534 
4535  if (Pol_em == 80. && Pol_ep == -30.){
4536  mu +=
4537  +120937. * CiHbox / LambdaNP2
4538  -41080.7 * CiHL1_11 / LambdaNP2
4539  -416801. * CiHe_11 / LambdaNP2
4540  -192794. * CiHL3_11 / LambdaNP2
4541  -182281. * CiHD / LambdaNP2
4542  +102909. * CiHB / LambdaNP2
4543  -87947.8 * CiHW / LambdaNP2
4544  -228111. * CiHWB / LambdaNP2
4545  +40181.7 * CiDHB / LambdaNP2
4546  -37530.5 * CiDHW / LambdaNP2
4547  -4.236 * DeltaGF()
4548  -4.832 * deltaMwd6()
4549  ;
4550 
4551  // Add modifications due to small variations of the SM parameters
4552  mu += cHSM * ( +3.177 * deltaMz()
4553  -1.894 * deltaMh()
4554  -0.171 * deltaaMZ()
4555  +3.022 * deltaGmu() );
4556 
4557  } else if (Pol_em == -80. && Pol_ep == 30.){
4558  mu +=
4559  +120796. * CiHbox / LambdaNP2
4560  -17710.6 * CiHL1_11 / LambdaNP2
4561  -1357.61 * CiHe_11 / LambdaNP2
4562  -241114. * CiHL3_11 / LambdaNP2
4563  -206464. * CiHD / LambdaNP2
4564  +5738.97 * CiHB / LambdaNP2
4565  -94600.4 * CiHW / LambdaNP2
4566  -387581. * CiHWB / LambdaNP2
4567  -1403.89 * CiDHB / LambdaNP2
4568  -31363.8 * CiDHW / LambdaNP2
4569  -4.699 * DeltaGF()
4570  -5.361 * deltaMwd6()
4571  ;
4572 
4573  // Add modifications due to small variations of the SM parameters
4574  mu += cHSM * ( +3.768 * deltaMz()
4575  -2. * deltaMh()
4576  -0.556 * deltaaMZ()
4577  +3.512 * deltaGmu() );
4578 
4579  } else if (Pol_em == 80. && Pol_ep == 0.){
4580  mu +=
4581  +121065. * CiHbox / LambdaNP2
4582  -30567.4 * CiHL1_11 / LambdaNP2
4583  -235832. * CiHe_11 / LambdaNP2
4584  -213581. * CiHL3_11 / LambdaNP2
4585  -192620. * CiHD / LambdaNP2
4586  +60320.1 * CiHB / LambdaNP2
4587  -90446.2 * CiHW / LambdaNP2
4588  -297833. * CiHWB / LambdaNP2
4589  +22132.1 * CiDHB / LambdaNP2
4590  -34844.4 * CiDHW / LambdaNP2
4591  -4.439 * DeltaGF()
4592  -5.054 * deltaMwd6()
4593  ;
4594 
4595  // Add modifications due to small variations of the SM parameters
4596  mu += cHSM * ( +3.437 * deltaMz()
4597  -1.943 * deltaMh()
4598  -0.343 * deltaaMZ()
4599  +3.237 * deltaGmu() );
4600 
4601  } else if (Pol_em == -80. && Pol_ep == 0.){
4602  mu +=
4603  +120725. * CiHbox / LambdaNP2
4604  -17741.9 * CiHL1_11 / LambdaNP2
4605  -2786.58 * CiHe_11 / LambdaNP2
4606  -241197. * CiHL3_11 / LambdaNP2
4607  -206387. * CiHD / LambdaNP2
4608  +6134.48 * CiHB / LambdaNP2
4609  -94603.3 * CiHW / LambdaNP2
4610  -387053. * CiHWB / LambdaNP2
4611  -1323.12 * CiDHB / LambdaNP2
4612  -31434.2 * CiDHW / LambdaNP2
4613  -4.696 * DeltaGF()
4614  -5.365 * deltaMwd6()
4615  ;
4616 
4617  // Add modifications due to small variations of the SM parameters
4618  mu += cHSM * ( +3.764 * deltaMz()
4619  -2. * deltaMh()
4620  -0.556 * deltaaMZ()
4621  +3.517 * deltaGmu() );
4622 
4623  } else {
4624  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
4625  }
4626 
4627  } else if (sqrt_s == 0.365) {
4628 
4629  C1 = 0.0062; // Use the same as 350 GeV
4630 
4631  if (Pol_em == 80. && Pol_ep == -30.){
4632  mu +=
4633  +121120. * CiHbox / LambdaNP2
4634  -43274.8 * CiHL1_11 / LambdaNP2
4635  -379332. * CiHe_11 / LambdaNP2
4636  -213151. * CiHL3_11 / LambdaNP2
4637  -185704. * CiHD / LambdaNP2
4638  +95027.9 * CiHB / LambdaNP2
4639  -87042.2 * CiHW / LambdaNP2
4640  -246839. * CiHWB / LambdaNP2
4641  +37834.6 * CiDHB / LambdaNP2
4642  -38594.2 * CiDHW / LambdaNP2
4643  -4.314 * DeltaGF()
4644  -4.867 * deltaMwd6()
4645  ;
4646 
4647  // Add modifications due to small variations of the SM parameters
4648  mu += cHSM * ( +3.356 * deltaMz()
4649  -1.787 * deltaMh()
4650  -0.246 * deltaaMZ()
4651  +3.12 * deltaGmu() );
4652 
4653  } else if (Pol_em == -80. && Pol_ep == 30.){
4654  mu +=
4655  +120708. * CiHbox / LambdaNP2
4656  -23163.4 * CiHL1_11 / LambdaNP2
4657  -1266.64 * CiHe_11 / LambdaNP2
4658  -256145. * CiHL3_11 / LambdaNP2
4659  -206112. * CiHD / LambdaNP2
4660  +7209.08 * CiHB / LambdaNP2
4661  -94095.3 * CiHW / LambdaNP2
4662  -386056. * CiHWB / LambdaNP2
4663  -673.745 * CiDHB / LambdaNP2
4664  -32528.4 * CiDHW / LambdaNP2
4665  -4.703 * DeltaGF()
4666  -5.297 * deltaMwd6()
4667  ;
4668 
4669  // Add modifications due to small variations of the SM parameters
4670  mu += cHSM * ( +3.865 * deltaMz()
4671  -1.869 * deltaMh()
4672  -0.577 * deltaaMZ()
4673  +3.533 * deltaGmu() );
4674 
4675  } else if (Pol_em == 80. && Pol_ep == 0.){
4676  mu +=
4677  +120872. * CiHbox / LambdaNP2
4678  -34492.1 * CiHL1_11 / LambdaNP2
4679  -212361. * CiHe_11 / LambdaNP2
4680  -232050. * CiHL3_11 / LambdaNP2
4681  -194801. * CiHD / LambdaNP2
4682  +56353. * CiHB / LambdaNP2
4683  -90080.9 * CiHW / LambdaNP2
4684  -308151. * CiHWB / LambdaNP2
4685  +20707.2 * CiDHB / LambdaNP2
4686  -35840.6 * CiDHW / LambdaNP2
4687  -4.485 * DeltaGF()
4688  -5.033 * deltaMwd6()
4689  ;
4690 
4691  // Add modifications due to small variations of the SM parameters
4692  mu += cHSM * ( +3.586 * deltaMz()
4693  -1.817 * deltaMh()
4694  -0.393 * deltaaMZ()
4695  +3.287 * deltaGmu() );
4696 
4697  } else if (Pol_em == -80. && Pol_ep == 0.){
4698  mu +=
4699  +120806. * CiHbox / LambdaNP2
4700  -23082.3 * CiHL1_11 / LambdaNP2
4701  -2521.89 * CiHe_11 / LambdaNP2
4702  -255807. * CiHL3_11 / LambdaNP2
4703  -205972. * CiHD / LambdaNP2
4704  +7600.7 * CiHB / LambdaNP2
4705  -94080.6 * CiHW / LambdaNP2
4706  -385587. * CiHWB / LambdaNP2
4707  -525.394 * CiDHB / LambdaNP2
4708  -32486.9 * CiDHW / LambdaNP2
4709  -4.703 * DeltaGF()
4710  -5.294 * deltaMwd6()
4711  ;
4712 
4713  // Add modifications due to small variations of the SM parameters
4714  mu += cHSM * ( +3.87 * deltaMz()
4715  -1.873 * deltaMh()
4716  -0.577 * deltaaMZ()
4717  +3.533 * deltaGmu() );
4718 
4719  } else {
4720  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
4721  }
4722 
4723  } else if (sqrt_s == 0.380) {
4724 
4725  C1 = 0.0062; // Use the same as 350 GeV
4726 
4727  if (Pol_em == 80. && Pol_ep == -30.){
4728  mu +=
4729  +120907. * CiHbox / LambdaNP2
4730  -43917.7 * CiHL1_11 / LambdaNP2
4731  -344628. * CiHe_11 / LambdaNP2
4732  -230932. * CiHL3_11 / LambdaNP2
4733  -188656. * CiHD / LambdaNP2
4734  +86802.5 * CiHB / LambdaNP2
4735  -86378.3 * CiHW / LambdaNP2
4736  -262732. * CiHWB / LambdaNP2
4737  +35211.7 * CiDHB / LambdaNP2
4738  -39122. * CiDHW / LambdaNP2
4739  -4.375 * DeltaGF()
4740  -4.833 * deltaMwd6()
4741  ;
4742 
4743  // Add modifications due to small variations of the SM parameters
4744  mu += cHSM * ( +3.526 * deltaMz()
4745  -1.675 * deltaMh()
4746  -0.322 * deltaaMZ()
4747  +3.202 * deltaGmu() );
4748 
4749  } else if (Pol_em == -80. && Pol_ep == 30.){
4750  mu +=
4751  +120826. * CiHbox / LambdaNP2
4752  -26397.1 * CiHL1_11 / LambdaNP2
4753  -1156.51 * CiHe_11 / LambdaNP2
4754  -268680. * CiHL3_11 / LambdaNP2
4755  -205752. * CiHD / LambdaNP2
4756  +8226.72 * CiHB / LambdaNP2
4757  -92973.9 * CiHW / LambdaNP2
4758  -384868. * CiHWB / LambdaNP2
4759  -154.996 * CiDHB / LambdaNP2
4760  -33479.2 * CiDHW / LambdaNP2
4761  -4.706 * DeltaGF()
4762  -5.24 * deltaMwd6()
4763  ;
4764 
4765  // Add modifications due to small variations of the SM parameters
4766  mu += cHSM * ( +3.957 * deltaMz()
4767  -1.756 * deltaMh()
4768  -0.592 * deltaaMZ()
4769  +3.551 * deltaGmu() );
4770 
4771  } else if (Pol_em == 80. && Pol_ep == 0.){
4772  mu +=
4773  +121123. * CiHbox / LambdaNP2
4774  -35934.5 * CiHL1_11 / LambdaNP2
4775  -191922. * CiHe_11 / LambdaNP2
4776  -247636. * CiHL3_11 / LambdaNP2
4777  -196255. * CiHD / LambdaNP2
4778  +52143.1 * CiHB / LambdaNP2
4779  -89227.7 * CiHW / LambdaNP2
4780  -317018. * CiHWB / LambdaNP2
4781  +19725.8 * CiDHB / LambdaNP2
4782  -36723.5 * CiDHW / LambdaNP2
4783  -4.524 * DeltaGF()
4784  -5.007 * deltaMwd6()
4785  ;
4786 
4787  // Add modifications due to small variations of the SM parameters
4788  mu += cHSM * ( +3.729 * deltaMz()
4789  -1.706 * deltaMh()
4790  -0.439 * deltaaMZ()
4791  +3.366 * deltaGmu() );
4792 
4793  } else if (Pol_em == -80. && Pol_ep == 0.){
4794  mu +=
4795  +120839. * CiHbox / LambdaNP2
4796  -26545. * CiHL1_11 / LambdaNP2
4797  -2293.44 * CiHe_11 / LambdaNP2
4798  -268673. * CiHL3_11 / LambdaNP2
4799  -205696. * CiHD / LambdaNP2
4800  +8476.41 * CiHB / LambdaNP2
4801  -92899.6 * CiHW / LambdaNP2
4802  -384414. * CiHWB / LambdaNP2
4803  +15.496 * CiDHB / LambdaNP2
4804  -33502.8 * CiDHW / LambdaNP2
4805  -4.704 * DeltaGF()
4806  -5.232 * deltaMwd6()
4807  ;
4808 
4809  // Add modifications due to small variations of the SM parameters
4810  mu += cHSM * ( +3.958 * deltaMz()
4811  -1.755 * deltaMh()
4812  -0.59 * deltaaMZ()
4813  +3.555 * deltaGmu() );
4814 
4815  } else {
4816  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
4817  }
4818 
4819  } else if (sqrt_s == 0.500) {
4820 
4821  C1 = 0.0061;
4822 
4823  if (Pol_em == 80. && Pol_ep == -30.){
4824  mu +=
4825  +120734. * CiHbox / LambdaNP2
4826  -33626. * CiHL1_11 / LambdaNP2
4827  -177471. * CiHe_11 / LambdaNP2
4828  -312922. * CiHL3_11 / LambdaNP2
4829  -199388. * CiHD / LambdaNP2
4830  +44288.8 * CiHB / LambdaNP2
4831  -78960.3 * CiHW / LambdaNP2
4832  -332501. * CiHWB / LambdaNP2
4833  +20615.5 * CiDHB / LambdaNP2
4834  -43923.9 * CiDHW / LambdaNP2
4835  -4.614 * DeltaGF()
4836  -4.84 * deltaMwd6()
4837  ;
4838 
4839  // Add modifications due to small variations of the SM parameters
4840  mu += cHSM * ( +4.296 * deltaMz()
4841  -1.178 * deltaMh()
4842  -0.582 * deltaaMZ()
4843  +3.535 * deltaGmu() );
4844 
4845  } else if (Pol_em == -80. && Pol_ep == 30.){
4846  mu +=
4847  +120746. * CiHbox / LambdaNP2
4848  -26369.8 * CiHL1_11 / LambdaNP2
4849  -905.141 * CiHe_11 / LambdaNP2
4850  -327709. * CiHL3_11 / LambdaNP2
4851  -204622. * CiHD / LambdaNP2
4852  +8508.33 * CiHB / LambdaNP2
4853  -82669.6 * CiHW / LambdaNP2
4854  -381185. * CiHWB / LambdaNP2
4855  +784.456 * CiDHB / LambdaNP2
4856  -41153.8 * CiDHW / LambdaNP2
4857  -4.711 * DeltaGF()
4858  -4.948 * deltaMwd6()
4859  ;
4860 
4861  // Add modifications due to small variations of the SM parameters
4862  mu += cHSM * ( +4.417 * deltaMz()
4863  -1.196 * deltaMh()
4864  -0.664 * deltaaMZ()
4865  +3.639 * deltaGmu() );
4866 
4867  } else if (Pol_em == 80. && Pol_ep == 0.){
4868  mu +=
4869  +120667. * CiHbox / LambdaNP2
4870  -30480.6 * CiHL1_11 / LambdaNP2
4871  -96672.9 * CiHe_11 / LambdaNP2
4872  -320011. * CiHL3_11 / LambdaNP2
4873  -201855. * CiHD / LambdaNP2
4874  +27690.6 * CiHB / LambdaNP2
4875  -80770. * CiHW / LambdaNP2
4876  -355060. * CiHWB / LambdaNP2
4877  +11299.4 * CiDHB / LambdaNP2
4878  -42756.5 * CiDHW / LambdaNP2
4879  -4.656 * DeltaGF()
4880  -4.875 * deltaMwd6()
4881  ;
4882 
4883  // Add modifications due to small variations of the SM parameters
4884  mu += cHSM * ( +4.345 * deltaMz()
4885  -1.186 * deltaMh()
4886  -0.621 * deltaaMZ()
4887  +3.589 * deltaGmu() );
4888 
4889  } else if (Pol_em == -80. && Pol_ep == 0.){
4890  mu +=
4891  +120715. * CiHbox / LambdaNP2
4892  -26433.4 * CiHL1_11 / LambdaNP2
4893  -1490.31 * CiHe_11 / LambdaNP2
4894  -327665. * CiHL3_11 / LambdaNP2
4895  -204644. * CiHD / LambdaNP2
4896  +8471.25 * CiHB / LambdaNP2
4897  -82673.2 * CiHW / LambdaNP2
4898  -381049. * CiHWB / LambdaNP2
4899  +862.813 * CiDHB / LambdaNP2
4900  -41179.7 * CiDHW / LambdaNP2
4901  -4.711 * DeltaGF()
4902  -4.942 * deltaMwd6()
4903  ;
4904 
4905  // Add modifications due to small variations of the SM parameters
4906  mu += cHSM * ( +4.416 * deltaMz()
4907  -1.194 * deltaMh()
4908  -0.664 * deltaaMZ()
4909  +3.64 * deltaGmu() );
4910 
4911  } else {
4912  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
4913  }
4914 
4915  } else if (sqrt_s == 1.0) {
4916 
4917  C1 = 0.0059;
4918 
4919  if (Pol_em == 80. && Pol_ep == -30.){
4920  mu +=
4921  +120494. * CiHbox / LambdaNP2
4922  -9728.66 * CiHL1_11 / LambdaNP2
4923  -46166.9 * CiHe_11 / LambdaNP2
4924  -452752. * CiHL3_11 / LambdaNP2
4925  -203700. * CiHD / LambdaNP2
4926  +8561.22 * CiHB / LambdaNP2
4927  -61449.7 * CiHW / LambdaNP2
4928  -374076. * CiHWB / LambdaNP2
4929  +6473.98 * CiDHB / LambdaNP2
4930  -64032.3 * CiDHW / LambdaNP2
4931  -4.706 * DeltaGF()
4932  -4.581 * deltaMwd6()
4933  ;
4934 
4935  // Add modifications due to small variations of the SM parameters
4936  mu += cHSM * ( +4.956 * deltaMz()
4937  -0.583 * deltaMh()
4938  -0.739 * deltaaMZ()
4939  +3.723 * deltaGmu() );
4940 
4941  } else if (Pol_em == -80. && Pol_ep == 30.){
4942  mu +=
4943  +120522. * CiHbox / LambdaNP2
4944  -8881.26 * CiHL1_11 / LambdaNP2
4945  -529.908 * CiHe_11 / LambdaNP2
4946  -454326. * CiHL3_11 / LambdaNP2
4947  -204057. * CiHD / LambdaNP2
4948  +3158.25 * CiHB / LambdaNP2
4949  -61850.9 * CiHW / LambdaNP2
4950  -380114. * CiHWB / LambdaNP2
4951  +63.589 * CiDHB / LambdaNP2
4952  -63800.9 * CiDHW / LambdaNP2
4953  -4.712 * DeltaGF()
4954  -4.587 * deltaMwd6()
4955  ;
4956 
4957  // Add modifications due to small variations of the SM parameters
4958  mu += cHSM * ( +4.967 * deltaMz()
4959  -0.582 * deltaMh()
4960  -0.746 * deltaaMZ()
4961  +3.731 * deltaGmu() );
4962 
4963  } else if (Pol_em == 80. && Pol_ep == -20.){
4964  mu +=
4965  +120541. * CiHbox / LambdaNP2
4966  -9598.71 * CiHL1_11 / LambdaNP2
4967  -37435. * CiHe_11 / LambdaNP2
4968  -453118. * CiHL3_11 / LambdaNP2
4969  -203771. * CiHD / LambdaNP2
4970  +7555.11 * CiHB / LambdaNP2
4971  -61524.6 * CiHW / LambdaNP2
4972  -375155. * CiHWB / LambdaNP2
4973  +5263.81 * CiDHB / LambdaNP2
4974  -64001.7 * CiDHW / LambdaNP2
4975  -4.706 * DeltaGF()
4976  -4.589 * deltaMwd6()
4977  ;
4978 
4979  // Add modifications due to small variations of the SM parameters
4980  mu += cHSM * ( +4.959 * deltaMz()
4981  -0.583 * deltaMh()
4982  -0.741 * deltaaMZ()
4983  +3.726 * deltaGmu() );
4984 
4985  } else if (Pol_em == -80. && Pol_ep == 20.){
4986  mu +=
4987  +120482. * CiHbox / LambdaNP2
4988  -8932.26 * CiHL1_11 / LambdaNP2
4989  -597.015 * CiHe_11 / LambdaNP2
4990  -454406. * CiHL3_11 / LambdaNP2
4991  -204110. * CiHD / LambdaNP2
4992  +3145.81 * CiHB / LambdaNP2
4993  -61837. * CiHW / LambdaNP2
4994  -380115. * CiHWB / LambdaNP2
4995  +45.924 * CiDHB / LambdaNP2
4996  -63834.7 * CiDHW / LambdaNP2
4997  -4.711 * DeltaGF()
4998  -4.588 * deltaMwd6()
4999  ;
5000 
5001  // Add modifications due to small variations of the SM parameters
5002  mu += cHSM * ( +4.968 * deltaMz()
5003  -0.582 * deltaMh()
5004  -0.746 * deltaaMZ()
5005  +3.73 * deltaGmu() );
5006 
5007  } else if (Pol_em == 80. && Pol_ep == 0.){
5008  mu +=
5009  +120509. * CiHbox / LambdaNP2
5010  -9342.32 * CiHL1_11 / LambdaNP2
5011  -25028.5 * CiHe_11 / LambdaNP2
5012  -453487. * CiHL3_11 / LambdaNP2
5013  -203871. * CiHD / LambdaNP2
5014  +6021.71 * CiHB / LambdaNP2
5015  -61580. * CiHW / LambdaNP2
5016  -376790. * CiHWB / LambdaNP2
5017  +3494.08 * CiDHB / LambdaNP2
5018  -63959. * CiDHW / LambdaNP2
5019  -4.708 * DeltaGF()
5020  -4.589 * deltaMwd6()
5021  ;
5022 
5023  // Add modifications due to small variations of the SM parameters
5024  mu += cHSM * ( +4.962 * deltaMz()
5025  -0.582 * deltaMh()
5026  -0.742 * deltaaMZ()
5027  +3.726 * deltaGmu() );
5028 
5029  } else if (Pol_em == -80. && Pol_ep == 0.){
5030  mu +=
5031  +120526. * CiHbox / LambdaNP2
5032  -8927.83 * CiHL1_11 / LambdaNP2
5033  -633.766 * CiHe_11 / LambdaNP2
5034  -454337. * CiHL3_11 / LambdaNP2
5035  -204073. * CiHD / LambdaNP2
5036  +3196.39 * CiHB / LambdaNP2
5037  -61833.5 * CiHW / LambdaNP2
5038  -380094. * CiHWB / LambdaNP2
5039  +82.665 * CiDHB / LambdaNP2
5040  -63817.5 * CiDHW / LambdaNP2
5041  -4.712 * DeltaGF()
5042  -4.588 * deltaMwd6()
5043  ;
5044 
5045  // Add modifications due to small variations of the SM parameters
5046  mu += cHSM * ( +4.967 * deltaMz()
5047  -0.582 * deltaMh()
5048  -0.746 * deltaaMZ()
5049  +3.731 * deltaGmu() );
5050 
5051  } else {
5052  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
5053  }
5054 
5055  } else if (sqrt_s == 1.4) {
5056 
5057  C1 = 0.0058;
5058 
5059  if (Pol_em == 80. && Pol_ep == -30.){
5060  mu +=
5061  +120516. * CiHbox / LambdaNP2
5062  -5019.36 * CiHL1_11 / LambdaNP2
5063  -29937.8 * CiHe_11 / LambdaNP2
5064  -521211. * CiHL3_11 / LambdaNP2
5065  -203908. * CiHD / LambdaNP2
5066  +4153.08 * CiHB / LambdaNP2
5067  -54219.3 * CiHW / LambdaNP2
5068  -377548. * CiHWB / LambdaNP2
5069  +4509.78 * CiDHB / LambdaNP2
5070  -76054.8 * CiDHW / LambdaNP2
5071  -4.71 * DeltaGF()
5072  -4.484 * deltaMwd6()
5073  ;
5074 
5075  // Add modifications due to small variations of the SM parameters
5076  mu += cHSM * ( +5.105 * deltaMz()
5077  -0.447 * deltaMh()
5078  -0.765 * deltaaMZ()
5079  +3.747 * deltaGmu() );
5080 
5081  } else if (Pol_em == -80. && Pol_ep == 30.){
5082  mu +=
5083  +120530. * CiHbox / LambdaNP2
5084  -4727.84 * CiHL1_11 / LambdaNP2
5085  -488.036 * CiHe_11 / LambdaNP2
5086  -521821. * CiHL3_11 / LambdaNP2
5087  -204045. * CiHD / LambdaNP2
5088  +1784.38 * CiHB / LambdaNP2
5089  -54507.5 * CiHW / LambdaNP2
5090  -380042. * CiHWB / LambdaNP2
5091  -122.009 * CiDHB / LambdaNP2
5092  -75950.5 * CiDHW / LambdaNP2
5093  -4.712 * DeltaGF()
5094  -4.487 * deltaMwd6()
5095  ;
5096 
5097  // Add modifications due to small variations of the SM parameters
5098  mu += cHSM * ( +5.108 * deltaMz()
5099  -0.447 * deltaMh()
5100  -0.768 * deltaaMZ()
5101  +3.749 * deltaGmu() );
5102 
5103  } else if (Pol_em == 80. && Pol_ep == 0.){
5104  mu +=
5105  +120542. * CiHbox / LambdaNP2
5106  -4870.22 * CiHL1_11 / LambdaNP2
5107  -16376.8 * CiHe_11 / LambdaNP2
5108  -521472. * CiHL3_11 / LambdaNP2
5109  -203960. * CiHD / LambdaNP2
5110  +3068.42 * CiHB / LambdaNP2
5111  -54375.2 * CiHW / LambdaNP2
5112  -378699. * CiHWB / LambdaNP2
5113  +2390.51 * CiDHB / LambdaNP2
5114  -75996.8 * CiDHW / LambdaNP2
5115  -4.711 * DeltaGF()
5116  -4.485 * deltaMwd6()
5117  ;
5118 
5119  // Add modifications due to small variations of the SM parameters
5120  mu += cHSM * ( +5.107 * deltaMz()
5121  -0.448 * deltaMh()
5122  -0.766 * deltaaMZ()
5123  +3.749 * deltaGmu() );
5124 
5125  } else if (Pol_em == -80. && Pol_ep == 0.){
5126  mu +=
5127  +120504. * CiHbox / LambdaNP2
5128  -4718.66 * CiHL1_11 / LambdaNP2
5129  -574.963 * CiHe_11 / LambdaNP2
5130  -521805. * CiHL3_11 / LambdaNP2
5131  -204053. * CiHD / LambdaNP2
5132  +1784.37 * CiHB / LambdaNP2
5133  -54482.7 * CiHW / LambdaNP2
5134  -380051. * CiHWB / LambdaNP2
5135  -99.132 * CiDHB / LambdaNP2
5136  -75974.5 * CiDHW / LambdaNP2
5137  -4.712 * DeltaGF()
5138  -4.487 * deltaMwd6()
5139  ;
5140 
5141  // Add modifications due to small variations of the SM parameters
5142  mu += cHSM * ( +5.107 * deltaMz()
5143  -0.447 * deltaMh()
5144  -0.767 * deltaaMZ()
5145  +3.749 * deltaGmu() );
5146 
5147  } else {
5148  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
5149  }
5150 
5151  } else if (sqrt_s == 1.5) {
5152 
5153  C1 = 0.0058;// Use the same as 1400 GeV
5154 
5155  if (Pol_em == 80. && Pol_ep == -30.){
5156  mu +=
5157  +120531. * CiHbox / LambdaNP2
5158  -4421.38 * CiHL1_11 / LambdaNP2
5159  -28114.2 * CiHe_11 / LambdaNP2
5160  -535633. * CiHL3_11 / LambdaNP2
5161  -203960. * CiHD / LambdaNP2
5162  +3556.32 * CiHB / LambdaNP2
5163  -52816.2 * CiHW / LambdaNP2
5164  -377932. * CiHWB / LambdaNP2
5165  +4253.17 * CiDHB / LambdaNP2
5166  -78599.6 * CiDHW / LambdaNP2
5167  -4.71 * DeltaGF()
5168  -4.465 * deltaMwd6()
5169  ;
5170 
5171  // Add modifications due to small variations of the SM parameters
5172  mu += cHSM * ( +5.128 * deltaMz()
5173  -0.424 * deltaMh()
5174  -0.772 * deltaaMZ()
5175  +3.755 * deltaGmu() );
5176 
5177  } else if (Pol_em == -80. && Pol_ep == 30.){
5178  mu +=
5179  +120491. * CiHbox / LambdaNP2
5180  -4113.21 * CiHL1_11 / LambdaNP2
5181  -517.747 * CiHe_11 / LambdaNP2
5182  -536169. * CiHL3_11 / LambdaNP2
5183  -204050. * CiHD / LambdaNP2
5184  +1553.24 * CiHB / LambdaNP2
5185  -53097.9 * CiHW / LambdaNP2
5186  -380055. * CiHWB / LambdaNP2
5187  -129.437 * CiDHB / LambdaNP2
5188  -78539.4 * CiDHW / LambdaNP2
5189  -4.711 * DeltaGF()
5190  -4.468 * deltaMwd6()
5191  ;
5192 
5193  // Add modifications due to small variations of the SM parameters
5194  mu += cHSM * ( +5.131 * deltaMz()
5195  -0.424 * deltaMh()
5196  -0.773 * deltaaMZ()
5197  +3.755 * deltaGmu() );
5198 
5199  } else if (Pol_em == 80. && Pol_ep == 0.){
5200  mu +=
5201  +120525. * CiHbox / LambdaNP2
5202  -4256.39 * CiHL1_11 / LambdaNP2
5203  -15376.9 * CiHe_11 / LambdaNP2
5204  -535845. * CiHL3_11 / LambdaNP2
5205  -203987. * CiHD / LambdaNP2
5206  +2641.32 * CiHB / LambdaNP2
5207  -53045.1 * CiHW / LambdaNP2
5208  -378920. * CiHWB / LambdaNP2
5209  +2237.55 * CiDHB / LambdaNP2
5210  -78549.8 * CiDHW / LambdaNP2
5211  -4.711 * DeltaGF()
5212  -4.468 * deltaMwd6()
5213  ;
5214 
5215  // Add modifications due to small variations of the SM parameters
5216  mu += cHSM * ( +5.129 * deltaMz()
5217  -0.424 * deltaMh()
5218  -0.772 * deltaaMZ()
5219  +3.753 * deltaGmu() );
5220 
5221  } else if (Pol_em == -80. && Pol_ep == 0.){
5222  mu +=
5223  +120499. * CiHbox / LambdaNP2
5224  -4113.23 * CiHL1_11 / LambdaNP2
5225  -616.984 * CiHe_11 / LambdaNP2
5226  -536155. * CiHL3_11 / LambdaNP2
5227  -204035. * CiHD / LambdaNP2
5228  +1570.5 * CiHB / LambdaNP2
5229  -53079.3 * CiHW / LambdaNP2
5230  -380043. * CiHWB / LambdaNP2
5231  -112.179 * CiDHB / LambdaNP2
5232  -78543.9 * CiDHW / LambdaNP2
5233  -4.711 * DeltaGF()
5234  -4.468 * deltaMwd6()
5235  ;
5236 
5237  // Add modifications due to small variations of the SM parameters
5238  mu += cHSM * ( +5.13 * deltaMz()
5239  -0.424 * deltaMh()
5240  -0.773 * deltaaMZ()
5241  +3.755 * deltaGmu() );
5242 
5243  } else {
5244  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
5245  }
5246 
5247  } else if (sqrt_s == 3.0) {
5248 
5249  C1 = 0.0057;
5250 
5251  if (Pol_em == 80. && Pol_ep == -30.){
5252  mu +=
5253  +120384. * CiHbox / LambdaNP2
5254  -1301.85 * CiHL1_11 / LambdaNP2
5255  -16370.4 * CiHe_11 / LambdaNP2
5256  -686389. * CiHL3_11 / LambdaNP2
5257  -204031. * CiHD / LambdaNP2
5258  +628.479 * CiHB / LambdaNP2
5259  -41464.7 * CiHW / LambdaNP2
5260  -379766. * CiHWB / LambdaNP2
5261  +2259.53 * CiDHB / LambdaNP2
5262  -104941. * CiDHW / LambdaNP2
5263  -4.706 * DeltaGF()
5264  -4.342 * deltaMwd6()
5265  ;
5266 
5267  // Add modifications due to small variations of the SM parameters
5268  mu += cHSM * ( +5.306 * deltaMz()
5269  -0.283 * deltaMh()
5270  -0.802 * deltaaMZ()
5271  +3.787 * deltaGmu() );
5272 
5273  } else if (Pol_em == -80. && Pol_ep == 30.){
5274  mu +=
5275  +120423. * CiHbox / LambdaNP2
5276  -1253.47 * CiHL1_11 / LambdaNP2
5277  -537.201 * CiHe_11 / LambdaNP2
5278  -686427. * CiHL3_11 / LambdaNP2
5279  -204047. * CiHD / LambdaNP2
5280  +268.601 * CiHB / LambdaNP2
5281  -41454. * CiHW / LambdaNP2
5282  -380141. * CiHWB / LambdaNP2
5283  -447.668 * CiDHB / LambdaNP2
5284  -104906. * CiDHW / LambdaNP2
5285  -4.707 * DeltaGF()
5286  -4.342 * deltaMwd6()
5287  ;
5288 
5289  // Add modifications due to small variations of the SM parameters
5290  mu += cHSM * ( +5.305 * deltaMz()
5291  -0.284 * deltaMh()
5292  -0.802 * deltaaMZ()
5293  +3.787 * deltaGmu() );
5294 
5295  } else if (Pol_em == 80. && Pol_ep == 0.){
5296  mu +=
5297  +120399. * CiHbox / LambdaNP2
5298  -1267.47 * CiHL1_11 / LambdaNP2
5299  -9008.44 * CiHe_11 / LambdaNP2
5300  -686485. * CiHL3_11 / LambdaNP2
5301  -204052. * CiHD / LambdaNP2
5302  +439.947 * CiHB / LambdaNP2
5303  -41459.8 * CiHW / LambdaNP2
5304  -379947. * CiHWB / LambdaNP2
5305  +1005.59 * CiDHB / LambdaNP2
5306  -104927. * CiDHW / LambdaNP2
5307  -4.706 * DeltaGF()
5308  -4.342 * deltaMwd6()
5309  ;
5310 
5311  // Add modifications due to small variations of the SM parameters
5312  mu += cHSM * ( +5.303 * deltaMz()
5313  -0.283 * deltaMh()
5314  -0.802 * deltaaMZ()
5315  +3.789 * deltaGmu() );
5316 
5317  } else if (Pol_em == -80. && Pol_ep == 0.){
5318  mu +=
5319  +120385. * CiHbox / LambdaNP2
5320  -1245.4 * CiHL1_11 / LambdaNP2
5321  -535.407 * CiHe_11 / LambdaNP2
5322  -686461. * CiHL3_11 / LambdaNP2
5323  -204048. * CiHD / LambdaNP2
5324  +244.425 * CiHB / LambdaNP2
5325  -41447.5 * CiHW / LambdaNP2
5326  -380150. * CiHWB / LambdaNP2
5327  -430.653 * CiDHB / LambdaNP2
5328  -104905. * CiDHW / LambdaNP2
5329  -4.706 * DeltaGF()
5330  -4.343 * deltaMwd6()
5331  ;
5332 
5333  // Add modifications due to small variations of the SM parameters
5334  mu += cHSM * ( +5.307 * deltaMz()
5335  -0.283 * deltaMh()
5336  -0.802 * deltaaMZ()
5337  +3.789 * deltaGmu() );
5338 
5339  } else {
5340  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
5341  }
5342 
5343  } else
5344  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
5345 
5346  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
5347  mu += eeeWBFint + eeeWBFpar;
5348 
5349 // Linear contribution from Higgs self-coupling
5350  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
5351 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
5353 
5354  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
5355 
5356  return mu;
5357 }

◆ mueettH()

double NPSMEFTd6::mueettH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{eettH}\)

Reimplemented from NPbase.

Definition at line 9005 of file NPSMEFTd6.cpp.

9006 {
9007  double mu = 1.0;
9008 
9009  double C1 = 0.0;
9010 
9011  if (sqrt_s == 0.500) {
9012 
9013  C1 = 0.086;
9014 
9015  mu +=
9016  +121901. * CiHbox / LambdaNP2
9017  +84038.2 * CiHL1_11 / LambdaNP2
9018  +41671.2 * CiHe_11 / LambdaNP2
9019  -31418.2 * CiHu_11 / LambdaNP2
9020  +84038.2 * CiHL3_11 / LambdaNP2
9021  -121791. * CiuH_33r / LambdaNP2
9022  -59467.6 * CiHD / LambdaNP2
9023  +138929. * CiHB / LambdaNP2
9024  +130909. * CiHW / LambdaNP2
9025  -253030. * CiHWB / LambdaNP2
9026  -1757.66 * CiDHB / LambdaNP2
9027  +1501.34 * CiDHW / LambdaNP2
9028  +1386027. * CiuW_33r / LambdaNP2
9029  +1698012. * CiuB_33r / LambdaNP2
9030  -1.965 * DeltaGF()
9031  -1.187 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9032  ;
9033 
9034  // Add modifications due to small variations of the SM parameters
9035  mu += cHSM * ( +1.932 * deltaMz()
9036  -9.827 * deltaMh()
9037  +1.04 * deltaaMZ()
9038  +1.992 * deltaGmu()
9039  -18.476 * deltamt() );
9040 
9041  if (FlagQuadraticTerms) {
9042  //Add contributions that are quadratic in the effective coefficients
9043  mu += 0.0;
9044  }
9045 
9046  } else if (sqrt_s == 1.0) {
9047 
9048  C1 = 0.017;
9049 
9050  mu +=
9051  +122013. * CiHbox / LambdaNP2
9052  +889282. * CiHL1_11 / LambdaNP2
9053  -543424. * CiHe_11 / LambdaNP2
9054  -8240.83 * CiHu_11 / LambdaNP2
9055  +889282. * CiHL3_11 / LambdaNP2
9056  -116099. * CiuH_33r / LambdaNP2
9057  -60351.9 * CiHD / LambdaNP2
9058  +352804. * CiHB / LambdaNP2
9059  +361918. * CiHW / LambdaNP2
9060  -397547. * CiHWB / LambdaNP2
9061  +37326.1 * CiDHB / LambdaNP2
9062  +113772. * CiDHW / LambdaNP2
9063  +2758980. * CiuW_33r / LambdaNP2
9064  +3462941. * CiuB_33r / LambdaNP2
9065  -2.08 * DeltaGF()
9066  -2.575 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9067  ;
9068 
9069  // Add modifications due to small variations of the SM parameters
9070  mu += cHSM * ( +2.185 * deltaMz()
9071  -1.195 * deltaMh()
9072  +0.92 * deltaaMZ()
9073  +2.096 * deltaGmu()
9074  +2.136 * deltamt() );
9075 
9076  if (FlagQuadraticTerms) {
9077  //Add contributions that are quadratic in the effective coefficients
9078  mu += 0.0;
9079  }
9080 
9081  } else if (sqrt_s == 1.4) {
9082 
9083  C1 = 0.0094;
9084 
9085  mu +=
9086  +122081. * CiHbox / LambdaNP2
9087  +2544832. * CiHL1_11 / LambdaNP2
9088  -1901938. * CiHe_11 / LambdaNP2
9089  +3241.73 * CiHu_11 / LambdaNP2
9090  +2544832. * CiHL3_11 / LambdaNP2
9091  -112208. * CiuH_33r / LambdaNP2
9092  -60340.4 * CiHD / LambdaNP2
9093  +464967. * CiHB / LambdaNP2
9094  +487659. * CiHW / LambdaNP2
9095  -471053. * CiHWB / LambdaNP2
9096  +134900. * CiDHB / LambdaNP2
9097  +371767. * CiDHW / LambdaNP2
9098  +3804096. * CiuW_33r / LambdaNP2
9099  +4800265. * CiuB_33r / LambdaNP2
9100  -2.139 * DeltaGF()
9101  -3.203 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9102  ;
9103 
9104  // Add modifications due to small variations of the SM parameters
9105  mu += cHSM * ( +2.309 * deltaMz()
9106  -0.898 * deltaMh()
9107  +0.872 * deltaaMZ()
9108  +2.157 * deltaGmu()
9109  +2.262 * deltamt() );
9110 
9111  if (FlagQuadraticTerms) {
9112  //Add contributions that are quadratic in the effective coefficients
9113  mu += 0.0;
9114  }
9115 
9116  } else if (sqrt_s == 1.5) {
9117 
9118  C1 = 0.0094;// Use the same as 1400 GeV
9119 
9120  mu +=
9121  +122173. * CiHbox / LambdaNP2
9122  +3117293. * CiHL1_11 / LambdaNP2
9123  -2378233. * CiHe_11 / LambdaNP2
9124  +5531.15 * CiHu_11 / LambdaNP2
9125  +3117293. * CiHL3_11 / LambdaNP2
9126  -111274. * CiuH_33r / LambdaNP2
9127  -60192. * CiHD / LambdaNP2
9128  +487962. * CiHB / LambdaNP2
9129  +513503. * CiHW / LambdaNP2
9130  -485782. * CiHWB / LambdaNP2
9131  +170734. * CiDHB / LambdaNP2
9132  +462665. * CiDHW / LambdaNP2
9133  +4068326. * CiuW_33r / LambdaNP2
9134  +5138930. * CiuB_33r / LambdaNP2
9135  -2.149 * DeltaGF()
9136  -3.325 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9137  ;
9138 
9139  // Add modifications due to small variations of the SM parameters
9140  mu += cHSM * ( +2.322 * deltaMz()
9141  -0.858 * deltaMh()
9142  +0.866 * deltaaMZ()
9143  +2.164 * deltaGmu()
9144  +2.265 * deltamt() );
9145 
9146  if (FlagQuadraticTerms) {
9147  //Add contributions that are quadratic in the effective coefficients
9148  mu += 0.0;
9149  }
9150 
9151  } else if (sqrt_s == 3.0) {
9152 
9153  C1 = 0.0037;
9154 
9155  mu +=
9156  +121915. * CiHbox / LambdaNP2
9157  +19529668. * CiHL1_11 / LambdaNP2
9158  -16356276. * CiHe_11 / LambdaNP2
9159  +23142.9 * CiHu_11 / LambdaNP2
9160  +19529668. * CiHL3_11 / LambdaNP2
9161  -104011. * CiuH_33r / LambdaNP2
9162  -58710.4 * CiHD / LambdaNP2
9163  +697868. * CiHB / LambdaNP2
9164  +751003. * CiHW / LambdaNP2
9165  -625171. * CiHWB / LambdaNP2
9166  +1204441. * CiDHB / LambdaNP2
9167  +3111413. * CiDHW / LambdaNP2
9168  +8604912. * CiuW_33r / LambdaNP2
9169  +10946841. * CiuB_33r / LambdaNP2
9170  -2.224 * DeltaGF()
9171  -4.279 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9172  ;
9173 
9174  // Add modifications due to small variations of the SM parameters
9175  mu += cHSM * ( +2.483 * deltaMz()
9176  -0.572 * deltaMh()
9177  +0.771 * deltaaMZ()
9178  +2.242 * deltaGmu()
9179  +2.182 * deltamt() );
9180 
9181  if (FlagQuadraticTerms) {
9182  //Add contributions that are quadratic in the effective coefficients
9183  mu += 0.0;
9184  }
9185 
9186  } else
9187  throw std::runtime_error("Bad argument in NPSMEFTd6::mueettH()");
9188 
9189  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
9190  mu += eeettHint + eeettHpar;
9191 
9192 // Linear contribution from Higgs self-coupling
9193  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
9194 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
9196 
9197  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
9198 
9199  return mu;
9200 }

◆ mueettHPol()

double NPSMEFTd6::mueettHPol ( const double  sqrt_s,
const double  Pol_em,
const double  Pol_ep 
) const
virtual

The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively
Returns
\(\mu_{eettH}\)

Reimplemented from NPbase.

Definition at line 9202 of file NPSMEFTd6.cpp.

9203 {
9204  double mu = 1.0;
9205 
9206  double C1 = 0.0;
9207 
9208  if (sqrt_s == 0.500) {
9209 
9210  C1 = 0.086;
9211 
9212  if (Pol_em == 80. && Pol_ep == -30.){
9213  mu +=
9214  +121861. * CiHbox / LambdaNP2
9215  +14207.9 * CiHL1_11 / LambdaNP2
9216  +124191. * CiHe_11 / LambdaNP2
9217  +112591. * CiHu_11 / LambdaNP2
9218  +14207.9 * CiHL3_11 / LambdaNP2
9219  -123399. * CiuH_33r / LambdaNP2
9220  -12437.7 * CiHD / LambdaNP2
9221  +249779. * CiHB / LambdaNP2
9222  +18912.8 * CiHW / LambdaNP2
9223  -109936. * CiHWB / LambdaNP2
9224  -5170.73 * CiDHB / LambdaNP2
9225  +3167.65 * CiDHW / LambdaNP2
9226  +174267. * CiuW_33r / LambdaNP2
9227  +3032981. * CiuB_33r / LambdaNP2
9228  -0.388 * DeltaGF()
9229  +3.51 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9230  ;
9231 
9232  // Add modifications due to small variations of the SM parameters
9233  mu += cHSM * ( -1.319 * deltaMz()
9234  -9.866 * deltaMh()
9235  +2.617 * deltaaMZ()
9236  +0.421 * deltaGmu()
9237  -18.44 * deltamt() );
9238 
9239  } else if (Pol_em == -80. && Pol_ep == 30.){
9240  mu +=
9241  +121809. * CiHbox / LambdaNP2
9242  +116253. * CiHL1_11 / LambdaNP2
9243  +3415.4 * CiHe_11 / LambdaNP2
9244  -98311.8 * CiHu_11 / LambdaNP2
9245  +116253. * CiHL3_11 / LambdaNP2
9246  -121117. * CiuH_33r / LambdaNP2
9247  -81321.2 * CiHD / LambdaNP2
9248  +87352.2 * CiHB / LambdaNP2
9249  +182702. * CiHW / LambdaNP2
9250  -319427. * CiHWB / LambdaNP2
9251  -21.616 * CiDHB / LambdaNP2
9252  +799.81 * CiDHW / LambdaNP2
9253  +1948272. * CiuW_33r / LambdaNP2
9254  +1078489. * CiuB_33r / LambdaNP2
9255  -2.697 * DeltaGF()
9256  -3.37 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9257  ;
9258 
9259  // Add modifications due to small variations of the SM parameters
9260  mu += cHSM * ( +3.441 * deltaMz()
9261  -9.806 * deltaMh()
9262  +0.308 * deltaaMZ()
9263  +2.725 * deltaGmu()
9264  -18.491 * deltamt() );
9265 
9266  } else if (Pol_em == 80. && Pol_ep == 0.){
9267  mu +=
9268  +121837. * CiHbox / LambdaNP2
9269  +24323.6 * CiHL1_11 / LambdaNP2
9270  +111998. * CiHe_11 / LambdaNP2
9271  +91391.1 * CiHu_11 / LambdaNP2
9272  +24323.6 * CiHL3_11 / LambdaNP2
9273  -123203. * CiuH_33r / LambdaNP2
9274  -19404.2 * CiHD / LambdaNP2
9275  +233452. * CiHB / LambdaNP2
9276  +35310.2 * CiHW / LambdaNP2
9277  -131019. * CiHWB / LambdaNP2
9278  -4810.06 * CiDHB / LambdaNP2
9279  +2842.31 * CiDHW / LambdaNP2
9280  +351790. * CiuW_33r / LambdaNP2
9281  +2837005. * CiuB_33r / LambdaNP2
9282  -0.617 * DeltaGF()
9283  +2.818 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9284  ;
9285 
9286  // Add modifications due to small variations of the SM parameters
9287  mu += cHSM * ( -0.843 * deltaMz()
9288  -9.86 * deltaMh()
9289  +2.385 * deltaaMZ()
9290  +0.645 * deltaGmu()
9291  -18.45 * deltamt() );
9292 
9293  } else if (Pol_em == -80. && Pol_ep == 0.){
9294  mu +=
9295  +121814. * CiHbox / LambdaNP2
9296  +113858. * CiHL1_11 / LambdaNP2
9297  +6221.44 * CiHe_11 / LambdaNP2
9298  -93321.6 * CiHu_11 / LambdaNP2
9299  +113858. * CiHL3_11 / LambdaNP2
9300  -121180. * CiuH_33r / LambdaNP2
9301  -79695. * CiHD / LambdaNP2
9302  +91201.9 * CiHB / LambdaNP2
9303  +178853. * CiHW / LambdaNP2
9304  -314513. * CiHWB / LambdaNP2
9305  -137.642 * CiDHB / LambdaNP2
9306  +853.383 * CiDHW / LambdaNP2
9307  +1906734. * CiuW_33r / LambdaNP2
9308  +1124181. * CiuB_33r / LambdaNP2
9309  -2.642 * DeltaGF()
9310  -3.21 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9311  ;
9312 
9313  // Add modifications due to small variations of the SM parameters
9314  mu += cHSM * ( +3.33 * deltaMz()
9315  -9.807 * deltaMh()
9316  +0.362 * deltaaMZ()
9317  +2.671 * deltaGmu()
9318  -18.489 * deltamt() );
9319 
9320  } else {
9321  throw std::runtime_error("Bad argument in NPSMEFTd6::mueettHPol()");
9322  }
9323 
9324  } else if (sqrt_s == 1.0) {
9325 
9326  C1 = 0.017;
9327 
9328  if (Pol_em == 80. && Pol_ep == -30.){
9329  mu +=
9330  +122269. * CiHbox / LambdaNP2
9331  +148925. * CiHL1_11 / LambdaNP2
9332  -1516295. * CiHe_11 / LambdaNP2
9333  +181376. * CiHu_11 / LambdaNP2
9334  +148925. * CiHL3_11 / LambdaNP2
9335  -115721. * CiuH_33r / LambdaNP2
9336  -9966.97 * CiHD / LambdaNP2
9337  +648027. * CiHB / LambdaNP2
9338  +58990.6 * CiHW / LambdaNP2
9339  -166947. * CiHWB / LambdaNP2
9340  +258446. * CiDHB / LambdaNP2
9341  +27641. * CiDHW / LambdaNP2
9342  +416063. * CiuW_33r / LambdaNP2
9343  +5771745. * CiuB_33r / LambdaNP2
9344  -0.426 * DeltaGF()
9345  +3.026 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9346  ;
9347 
9348  // Add modifications due to small variations of the SM parameters
9349  mu += cHSM * ( -1.159 * deltaMz()
9350  -1.211 * deltaMh()
9351  +2.586 * deltaaMZ()
9352  +0.445 * deltaGmu()
9353  +2.101 * deltamt() );
9354 
9355  } else if (Pol_em == -80. && Pol_ep == 30.){
9356  mu +=
9357  +122212. * CiHbox / LambdaNP2
9358  +1266376. * CiHL1_11 / LambdaNP2
9359  -47326.8 * CiHe_11 / LambdaNP2
9360  -104685. * CiHu_11 / LambdaNP2
9361  +1266376. * CiHL3_11 / LambdaNP2
9362  -116193. * CiuH_33r / LambdaNP2
9363  -85861. * CiHD / LambdaNP2
9364  +202732. * CiHB / LambdaNP2
9365  +516612. * CiHW / LambdaNP2
9366  -514723. * CiHWB / LambdaNP2
9367  -75504.5 * CiDHB / LambdaNP2
9368  +158356. * CiDHW / LambdaNP2
9369  +3954267. * CiuW_33r / LambdaNP2
9370  +2288387. * CiuB_33r / LambdaNP2
9371  -2.929 * DeltaGF()
9372  -5.432 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9373  ;
9374 
9375  // Add modifications due to small variations of the SM parameters
9376  mu += cHSM * ( +3.902 * deltaMz()
9377  -1.192 * deltaMh()
9378  +0.075 * deltaaMZ()
9379  +2.94 * deltaGmu()
9380  +2.16 * deltamt() );
9381 
9382  } else if (Pol_em == 80. && Pol_ep == -20.){
9383  mu +=
9384  +122563. * CiHbox / LambdaNP2
9385  +179718. * CiHL1_11 / LambdaNP2
9386  -1476392. * CiHe_11 / LambdaNP2
9387  +173910. * CiHu_11 / LambdaNP2
9388  +179718. * CiHL3_11 / LambdaNP2
9389  -115349. * CiuH_33r / LambdaNP2
9390  -11797.8 * CiHD / LambdaNP2
9391  +636347. * CiHB / LambdaNP2
9392  +71703.6 * CiHW / LambdaNP2
9393  -176417. * CiHWB / LambdaNP2
9394  +249649. * CiDHB / LambdaNP2
9395  +31542.3 * CiDHW / LambdaNP2
9396  +513357. * CiuW_33r / LambdaNP2
9397  +5678281. * CiuB_33r / LambdaNP2
9398  -0.497 * DeltaGF()
9399  +2.823 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9400  ;
9401 
9402  // Add modifications due to small variations of the SM parameters
9403  mu += cHSM * ( -0.986 * deltaMz()
9404  -1.242 * deltaMh()
9405  +2.514 * deltaaMZ()
9406  +0.529 * deltaGmu()
9407  +2.133 * deltamt() );
9408 
9409  } else if (Pol_em == -80. && Pol_ep == 20.){
9410  mu +=
9411  +122316. * CiHbox / LambdaNP2
9412  +1258544. * CiHL1_11 / LambdaNP2
9413  -57807.1 * CiHe_11 / LambdaNP2
9414  -102560. * CiHu_11 / LambdaNP2
9415  +1258544. * CiHL3_11 / LambdaNP2
9416  -116091. * CiuH_33r / LambdaNP2
9417  -85249.7 * CiHD / LambdaNP2
9418  +206295. * CiHB / LambdaNP2
9419  +513404. * CiHW / LambdaNP2
9420  -512197. * CiHWB / LambdaNP2
9421  -72925.9 * CiDHB / LambdaNP2
9422  +157286. * CiDHW / LambdaNP2
9423  +3929488. * CiuW_33r / LambdaNP2
9424  +2314064. * CiuB_33r / LambdaNP2
9425  -2.911 * DeltaGF()
9426  -5.37 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9427  ;
9428 
9429  // Add modifications due to small variations of the SM parameters
9430  mu += cHSM * ( +3.877 * deltaMz()
9431  -1.222 * deltaMh()
9432  +0.099 * deltaaMZ()
9433  +2.937 * deltaGmu()
9434  +2.184 * deltamt() );
9435 
9436  } else if (Pol_em == 80. && Pol_ep == 0.){
9437  mu +=
9438  +122564. * CiHbox / LambdaNP2
9439  +252265. * CiHL1_11 / LambdaNP2
9440  -1381101. * CiHe_11 / LambdaNP2
9441  +155161. * CiHu_11 / LambdaNP2
9442  +252265. * CiHL3_11 / LambdaNP2
9443  -115358. * CiuH_33r / LambdaNP2
9444  -16813.1 * CiHD / LambdaNP2
9445  +607466. * CiHB / LambdaNP2
9446  +101359. * CiHW / LambdaNP2
9447  -198737. * CiHWB / LambdaNP2
9448  +227834. * CiDHB / LambdaNP2
9449  +39939.6 * CiDHW / LambdaNP2
9450  +742520. * CiuW_33r / LambdaNP2
9451  +5453267. * CiuB_33r / LambdaNP2
9452  -0.659 * DeltaGF()
9453  +2.273 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9454  ;
9455 
9456  // Add modifications due to small variations of the SM parameters
9457  mu += cHSM * ( -0.69 * deltaMz()
9458  -1.205 * deltaMh()
9459  +2.349 * deltaaMZ()
9460  +0.676 * deltaGmu()
9461  +2.105 * deltamt() );
9462 
9463  } else if (Pol_em == -80. && Pol_ep == 0.){
9464  mu +=
9465  +122380. * CiHbox / LambdaNP2
9466  +1238124. * CiHL1_11 / LambdaNP2
9467  -84811.2 * CiHe_11 / LambdaNP2
9468  -97259.2 * CiHu_11 / LambdaNP2
9469  +1238124. * CiHL3_11 / LambdaNP2
9470  -116044. * CiuH_33r / LambdaNP2
9471  -83798.9 * CiHD / LambdaNP2
9472  +214128. * CiHB / LambdaNP2
9473  +505118. * CiHW / LambdaNP2
9474  -505830. * CiHWB / LambdaNP2
9475  -66814.1 * CiDHB / LambdaNP2
9476  +155075. * CiDHW / LambdaNP2
9477  +3863710. * CiuW_33r / LambdaNP2
9478  +2378351. * CiuB_33r / LambdaNP2
9479  -2.867 * DeltaGF()
9480  -5.212 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9481  ;
9482 
9483  // Add modifications due to small variations of the SM parameters
9484  mu += cHSM * ( +3.771 * deltaMz()
9485  -1.195 * deltaMh()
9486  +0.137 * deltaaMZ()
9487  +2.878 * deltaGmu()
9488  +2.166 * deltamt() );
9489 
9490  } else {
9491  throw std::runtime_error("Bad argument in NPSMEFTd6::mueettHPol()");
9492  }
9493 
9494  } else if (sqrt_s == 1.4) {
9495 
9496  C1 = 0.0094;
9497 
9498  if (Pol_em == 80. && Pol_ep == -30.){
9499  mu +=
9500  +121945. * CiHbox / LambdaNP2
9501  +416437. * CiHL1_11 / LambdaNP2
9502  -5198451. * CiHe_11 / LambdaNP2
9503  +211446. * CiHu_11 / LambdaNP2
9504  +416437. * CiHL3_11 / LambdaNP2
9505  -110413. * CiuH_33r / LambdaNP2
9506  -8089.5 * CiHD / LambdaNP2
9507  +852065. * CiHB / LambdaNP2
9508  +78915.7 * CiHW / LambdaNP2
9509  -191411. * CiHWB / LambdaNP2
9510  +881670. * CiDHB / LambdaNP2
9511  +72289.2 * CiDHW / LambdaNP2
9512  +588296. * CiuW_33r / LambdaNP2
9513  +7812392. * CiuB_33r / LambdaNP2
9514  -0.441 * DeltaGF()
9515  +2.819 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9516  ;
9517 
9518  // Add modifications due to small variations of the SM parameters
9519  mu += cHSM * ( -1.109 * deltaMz()
9520  -0.905 * deltaMh()
9521  +2.571 * deltaaMZ()
9522  +0.451 * deltaGmu()
9523  +2.225 * deltamt() );
9524 
9525  } else if (Pol_em == -80. && Pol_ep == 30.){
9526  mu +=
9527  +122124. * CiHbox / LambdaNP2
9528  +3668482. * CiHL1_11 / LambdaNP2
9529  -164738. * CiHe_11 / LambdaNP2
9530  -106285. * CiHu_11 / LambdaNP2
9531  +3668482. * CiHL3_11 / LambdaNP2
9532  -112775. * CiuH_33r / LambdaNP2
9533  -87497.2 * CiHD / LambdaNP2
9534  +261266. * CiHB / LambdaNP2
9535  +703789. * CiHW / LambdaNP2
9536  -618584. * CiHWB / LambdaNP2
9537  -257636. * CiDHB / LambdaNP2
9538  +530202. * CiDHW / LambdaNP2
9539  +5501929. * CiuW_33r / LambdaNP2
9540  +3213842. * CiuB_33r / LambdaNP2
9541  -3.038 * DeltaGF()
9542  -6.378 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9543  ;
9544 
9545  // Add modifications due to small variations of the SM parameters
9546  mu += cHSM * ( +4.12 * deltaMz()
9547  -0.898 * deltaMh()
9548  -0.029 * deltaaMZ()
9549  +3.056 * deltaGmu()
9550  +2.28 * deltamt() );
9551 
9552  } else if (Pol_em == 80. && Pol_ep == 0.){
9553  mu +=
9554  +121843. * CiHbox / LambdaNP2
9555  +706068. * CiHL1_11 / LambdaNP2
9556  -4748505. * CiHe_11 / LambdaNP2
9557  +182964. * CiHu_11 / LambdaNP2
9558  +706068. * CiHL3_11 / LambdaNP2
9559  -110672. * CiuH_33r / LambdaNP2
9560  -15249.5 * CiHD / LambdaNP2
9561  +798771. * CiHB / LambdaNP2
9562  +134415. * CiHW / LambdaNP2
9563  -229663. * CiHWB / LambdaNP2
9564  +779863. * CiDHB / LambdaNP2
9565  +112951. * CiDHW / LambdaNP2
9566  +1026697. * CiuW_33r / LambdaNP2
9567  +7402171. * CiuB_33r / LambdaNP2
9568  -0.673 * DeltaGF()
9569  +1.996 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9570  ;
9571 
9572  // Add modifications due to small variations of the SM parameters
9573  mu += cHSM * ( -0.648 * deltaMz()
9574  -0.901 * deltaMh()
9575  +2.34 * deltaaMZ()
9576  +0.693 * deltaGmu()
9577  +2.232 * deltamt() );
9578 
9579  } else if (Pol_em == -80. && Pol_ep == 0.){
9580  mu +=
9581  +122069. * CiHbox / LambdaNP2
9582  +3581543. * CiHL1_11 / LambdaNP2
9583  -298692. * CiHe_11 / LambdaNP2
9584  -97874.3 * CiHu_11 / LambdaNP2
9585  +3581543. * CiHL3_11 / LambdaNP2
9586  -112737. * CiuH_33r / LambdaNP2
9587  -85431.2 * CiHD / LambdaNP2
9588  +276629. * CiHB / LambdaNP2
9589  +687136. * CiHW / LambdaNP2
9590  -607155. * CiHWB / LambdaNP2
9591  -227375. * CiDHB / LambdaNP2
9592  +517945. * CiDHW / LambdaNP2
9593  +5370183. * CiuW_33r / LambdaNP2
9594  +3335906. * CiuB_33r / LambdaNP2
9595  -2.969 * DeltaGF()
9596  -6.138 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9597  ;
9598 
9599  // Add modifications due to small variations of the SM parameters
9600  mu += cHSM * ( +3.976 * deltaMz()
9601  -0.895 * deltaMh()
9602  +0.039 * deltaaMZ()
9603  +2.986 * deltaGmu()
9604  +2.271 * deltamt() );
9605 
9606  } else {
9607  throw std::runtime_error("Bad argument in NPSMEFTd6::mueettHPol()");
9608  }
9609 
9610  } else if (sqrt_s == 1.5) {
9611 
9612  C1 = 0.0094;// Use the same as 1400 GeV
9613 
9614  if (Pol_em == 80. && Pol_ep == -30.){
9615  mu +=
9616  +121854. * CiHbox / LambdaNP2
9617  +507190. * CiHL1_11 / LambdaNP2
9618  -6475118. * CiHe_11 / LambdaNP2
9619  +216935. * CiHu_11 / LambdaNP2
9620  +507190. * CiHL3_11 / LambdaNP2
9621  -109820. * CiuH_33r / LambdaNP2
9622  -7568.59 * CiHD / LambdaNP2
9623  +893094. * CiHB / LambdaNP2
9624  +82781.5 * CiHW / LambdaNP2
9625  -196556. * CiHWB / LambdaNP2
9626  +1099527. * CiDHB / LambdaNP2
9627  +87228. * CiDHW / LambdaNP2
9628  +630747. * CiuW_33r / LambdaNP2
9629  +8328477. * CiuB_33r / LambdaNP2
9630  -0.442 * DeltaGF()
9631  +2.756 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9632  ;
9633 
9634  // Add modifications due to small variations of the SM parameters
9635  mu += cHSM * ( -1.104 * deltaMz()
9636  -0.856 * deltaMh()
9637  +2.568 * deltaaMZ()
9638  +0.455 * deltaGmu()
9639  +2.232 * deltamt() );
9640 
9641  } else if (Pol_em == -80. && Pol_ep == 30.){
9642  mu +=
9643  +121994. * CiHbox / LambdaNP2
9644  +4501280. * CiHL1_11 / LambdaNP2
9645  -206085. * CiHe_11 / LambdaNP2
9646  -106381. * CiHu_11 / LambdaNP2
9647  +4501280. * CiHL3_11 / LambdaNP2
9648  -112104. * CiuH_33r / LambdaNP2
9649  -87805.6 * CiHD / LambdaNP2
9650  +273106. * CiHB / LambdaNP2
9651  +741955. * CiHW / LambdaNP2
9652  -639545. * CiHWB / LambdaNP2
9653  -322155. * CiDHB / LambdaNP2
9654  +661931. * CiDHW / LambdaNP2
9655  +5892414. * CiuW_33r / LambdaNP2
9656  +3448015. * CiuB_33r / LambdaNP2
9657  -3.057 * DeltaGF()
9658  -6.552 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9659  ;
9660 
9661  // Add modifications due to small variations of the SM parameters
9662  mu += cHSM * ( +4.154 * deltaMz()
9663  -0.856 * deltaMh()
9664  -0.045 * deltaaMZ()
9665  +3.071 * deltaGmu()
9666  +2.287 * deltamt() );
9667 
9668  } else if (Pol_em == 80. && Pol_ep == 0.){
9669  mu +=
9670  +121793. * CiHbox / LambdaNP2
9671  +861242. * CiHL1_11 / LambdaNP2
9672  -5919951. * CiHe_11 / LambdaNP2
9673  +188249. * CiHu_11 / LambdaNP2
9674  +861242. * CiHL3_11 / LambdaNP2
9675  -109696. * CiuH_33r / LambdaNP2
9676  -14806.7 * CiHD / LambdaNP2
9677  +837632. * CiHB / LambdaNP2
9678  +141142. * CiHW / LambdaNP2
9679  -235907. * CiHWB / LambdaNP2
9680  +973107. * CiDHB / LambdaNP2
9681  +138331. * CiDHW / LambdaNP2
9682  +1097452. * CiuW_33r / LambdaNP2
9683  +7895510. * CiuB_33r / LambdaNP2
9684  -0.673 * DeltaGF()
9685  +1.935 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9686  ;
9687 
9688  // Add modifications due to small variations of the SM parameters
9689  mu += cHSM * ( -0.637 * deltaMz()
9690  -0.859 * deltaMh()
9691  +2.339 * deltaaMZ()
9692  +0.68 * deltaGmu()
9693  +2.236 * deltamt() );
9694 
9695  } else if (Pol_em == -80. && Pol_ep == 0.){
9696  mu +=
9697  +122029. * CiHbox / LambdaNP2
9698  +4394189. * CiHL1_11 / LambdaNP2
9699  -373205. * CiHe_11 / LambdaNP2
9700  -97750.6 * CiHu_11 / LambdaNP2
9701  +4394189. * CiHL3_11 / LambdaNP2
9702  -112024. * CiuH_33r / LambdaNP2
9703  -85643.3 * CiHD / LambdaNP2
9704  +289620. * CiHB / LambdaNP2
9705  +724463. * CiHW / LambdaNP2
9706  -627885. * CiHWB / LambdaNP2
9707  -284076. * CiDHB / LambdaNP2
9708  +646658. * CiDHW / LambdaNP2
9709  +5753330. * CiuW_33r / LambdaNP2
9710  +3578793. * CiuB_33r / LambdaNP2
9711  -2.989 * DeltaGF()
9712  -6.311 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9713  ;
9714 
9715  // Add modifications due to small variations of the SM parameters
9716  mu += cHSM * ( +4.014 * deltaMz()
9717  -0.855 * deltaMh()
9718  +0.024 * deltaaMZ()
9719  +3.011 * deltaGmu()
9720  +2.286 * deltamt() );
9721 
9722  } else {
9723  throw std::runtime_error("Bad argument in NPSMEFTd6::mueettHPol()");
9724  }
9725 
9726  } else if (sqrt_s == 3.0) {
9727 
9728  C1 = 0.0037;
9729 
9730  if (Pol_em == 80. && Pol_ep == -30.){
9731  mu +=
9732  +122442. * CiHbox / LambdaNP2
9733  +3092340. * CiHL1_11 / LambdaNP2
9734  -43264264. * CiHe_11 / LambdaNP2
9735  +259622. * CiHu_11 / LambdaNP2
9736  +3092340. * CiHL3_11 / LambdaNP2
9737  -100510. * CiuH_33r / LambdaNP2
9738  -3230.01 * CiHD / LambdaNP2
9739  +1267548. * CiHB / LambdaNP2
9740  +118886. * CiHW / LambdaNP2
9741  -247164. * CiHWB / LambdaNP2
9742  +7397753. * CiDHB / LambdaNP2
9743  +510206. * CiDHW / LambdaNP2
9744  +1343630. * CiuW_33r / LambdaNP2
9745  +17234081. * CiuB_33r / LambdaNP2
9746  -0.459 * DeltaGF()
9747  +2.453 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9748  ;
9749 
9750  // Add modifications due to small variations of the SM parameters
9751  mu += cHSM * ( -1.07 * deltaMz()
9752  -0.576 * deltaMh()
9753  +2.542 * deltaaMZ()
9754  +0.468 * deltaGmu()
9755  +2.145 * deltamt() );
9756 
9757  } else if (Pol_em == -80. && Pol_ep == 30.){
9758  mu +=
9759  +122230. * CiHbox / LambdaNP2
9760  +28686134. * CiHL1_11 / LambdaNP2
9761  -1435177. * CiHe_11 / LambdaNP2
9762  -108195. * CiHu_11 / LambdaNP2
9763  +28686134. * CiHL3_11 / LambdaNP2
9764  -105858. * CiuH_33r / LambdaNP2
9765  -89803.1 * CiHD / LambdaNP2
9766  +381886. * CiHB / LambdaNP2
9767  +1102843. * CiHW / LambdaNP2
9768  -834821. * CiHWB / LambdaNP2
9769  -2237555. * CiDHB / LambdaNP2
9770  +4557030. * CiDHW / LambdaNP2
9771  +12639913. * CiuW_33r / LambdaNP2
9772  +7455995. * CiuB_33r / LambdaNP2
9773  -3.212 * DeltaGF()
9774  -8.009 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9775  ;
9776 
9777  // Add modifications due to small variations of the SM parameters
9778  mu += cHSM * ( +4.469 * deltaMz()
9779  -0.595 * deltaMh()
9780  -0.222 * deltaaMZ()
9781  +3.22 * deltaGmu()
9782  +2.195 * deltamt() );
9783 
9784  } else if (Pol_em == 80. && Pol_ep == 0.){
9785  mu +=
9786  +122688. * CiHbox / LambdaNP2
9787  +5271741. * CiHL1_11 / LambdaNP2
9788  -39707692. * CiHe_11 / LambdaNP2
9789  +228729. * CiHu_11 / LambdaNP2
9790  +5271741. * CiHL3_11 / LambdaNP2
9791  -100891. * CiuH_33r / LambdaNP2
9792  -10526.3 * CiHD / LambdaNP2
9793  +1192421. * CiHB / LambdaNP2
9794  +202915. * CiHW / LambdaNP2
9795  -296939. * CiHWB / LambdaNP2
9796  +6582510. * CiDHB / LambdaNP2
9797  +853895. * CiDHW / LambdaNP2
9798  +2303644. * CiuW_33r / LambdaNP2
9799  +16407287. * CiuB_33r / LambdaNP2
9800  -0.693 * DeltaGF()
9801  +1.565 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9802  ;
9803 
9804  // Add modifications due to small variations of the SM parameters
9805  mu += cHSM * ( -0.597 * deltaMz()
9806  -0.565 * deltaMh()
9807  +2.305 * deltaaMZ()
9808  +0.708 * deltaGmu()
9809  +2.153 * deltamt() );
9810 
9811  } else if (Pol_em == -80. && Pol_ep == 0.){
9812  mu +=
9813  +121781. * CiHbox / LambdaNP2
9814  +27966374. * CiHL1_11 / LambdaNP2
9815  -2597153. * CiHe_11 / LambdaNP2
9816  -98089.4 * CiHu_11 / LambdaNP2
9817  +27966374. * CiHL3_11 / LambdaNP2
9818  -105885. * CiuH_33r / LambdaNP2
9819  -87600.3 * CiHD / LambdaNP2
9820  +406305. * CiHB / LambdaNP2
9821  +1075086. * CiHW / LambdaNP2
9822  -818808. * CiHWB / LambdaNP2
9823  -1967062. * CiDHB / LambdaNP2
9824  +4442109. * CiDHW / LambdaNP2
9825  +12322125. * CiuW_33r / LambdaNP2
9826  +7728315. * CiuB_33r / LambdaNP2
9827  -3.134 * DeltaGF()
9828  -7.724 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9829  ;
9830 
9831  // Add modifications due to small variations of the SM parameters
9832  mu += cHSM * ( +4.305 * deltaMz()
9833  -0.59 * deltaMh()
9834  -0.147 * deltaaMZ()
9835  +3.144 * deltaGmu()
9836  +2.192 * deltamt() );
9837 
9838  } else {
9839  throw std::runtime_error("Bad argument in NPSMEFTd6::mueettHPol()");
9840  }
9841 
9842  } else
9843  throw std::runtime_error("Bad argument in NPSMEFTd6::mueettHPol()");
9844 
9845  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
9846  mu += eeettHint + eeettHpar;
9847 
9848 // Linear contribution from Higgs self-coupling
9849  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
9850 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
9852 
9853  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
9854 
9855  return mu;
9856 }

◆ mueeWBF()

double NPSMEFTd6::mueeWBF ( const double  sqrt_s) const
virtual

The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{eeWBF}\)

Reimplemented from NPbase.

Definition at line 3694 of file NPSMEFTd6.cpp.

3695 {
3696  double mu = 1.0;
3697 
3698  double C1 = 0.0;
3699 
3700  if (sqrt_s == 0.240) {
3701 
3702  C1 = 0.0064;
3703 
3704  mu +=
3705  +121120. * CiHbox / LambdaNP2
3706  -138682. * CiHL3_11 / LambdaNP2
3707  -203727. * CiHD / LambdaNP2
3708  -24699.7 * CiHW / LambdaNP2
3709  -379830. * CiHWB / LambdaNP2
3710  -18173.7 * CiDHW / LambdaNP2
3711  -4.716 * DeltaGF()
3712  -5.665 * deltaMwd6()
3713  ;
3714 
3715  // Add modifications due to small variations of the SM parameters
3716  mu += cHSM * (
3717  +3.307 * deltaMz()
3718  -3.995 * deltaMh()
3719  -0.486 * deltaaMZ()
3720  +3.507 * deltaGmu() );
3721 
3722  if (FlagQuadraticTerms) {
3723  //Add contributions that are quadratic in the effective coefficients
3724  mu += 0.0;
3725  }
3726 
3727  } else if (sqrt_s == 0.250) {
3728 
3729  C1 = 0.0064;
3730 
3731  mu +=
3732  +121142. * CiHbox / LambdaNP2
3733  -147357. * CiHL3_11 / LambdaNP2
3734  -203726. * CiHD / LambdaNP2
3735  -26559.2 * CiHW / LambdaNP2
3736  -379797. * CiHWB / LambdaNP2
3737  -19265.3 * CiDHW / LambdaNP2
3738  -4.717 * DeltaGF()
3739  -5.593 * deltaMwd6()
3740  ;
3741 
3742  // Add modifications due to small variations of the SM parameters
3743  mu += cHSM * (
3744  +3.413 * deltaMz()
3745  -3.644 * deltaMh()
3746  -0.502 * deltaaMZ()
3747  +3.523 * deltaGmu() );
3748 
3749  if (FlagQuadraticTerms) {
3750  //Add contributions that are quadratic in the effective coefficients
3751  mu += 0.0;
3752  }
3753 
3754  } else if (sqrt_s == 0.350) {
3755 
3756  C1 = 0.0062;
3757 
3758  mu +=
3759  +121107. * CiHbox / LambdaNP2
3760  -219582. * CiHL3_11 / LambdaNP2
3761  -203717. * CiHD / LambdaNP2
3762  -39722.3 * CiHW / LambdaNP2
3763  -379795. * CiHWB / LambdaNP2
3764  -28864.2 * CiDHW / LambdaNP2
3765  -4.714 * DeltaGF()
3766  -5.13 * deltaMwd6()
3767  ;
3768 
3769  // Add modifications due to small variations of the SM parameters
3770  mu += cHSM * (
3771  +4.073 * deltaMz()
3772  -1.94 * deltaMh()
3773  -0.598 * deltaaMZ()
3774  +3.623 * deltaGmu() );
3775 
3776  if (FlagQuadraticTerms) {
3777  //Add contributions that are quadratic in the effective coefficients
3778  mu += 0.0;
3779  }
3780 
3781  } else if (sqrt_s == 0.365) {
3782 
3783  C1 = 0.0062; // Use the same as 350 GeV
3784 
3785  mu +=
3786  +121071. * CiHbox / LambdaNP2
3787  -228452. * CiHL3_11 / LambdaNP2
3788  -203725. * CiHD / LambdaNP2
3789  -40966.9 * CiHW / LambdaNP2
3790  -379798. * CiHWB / LambdaNP2
3791  -30110.4 * CiDHW / LambdaNP2
3792  -4.714 * DeltaGF()
3793  -5.08 * deltaMwd6()
3794  ;
3795 
3796  // Add modifications due to small variations of the SM parameters
3797  mu += cHSM * (
3798  +4.136 * deltaMz()
3799  -1.817 * deltaMh()
3800  -0.609 * deltaaMZ()
3801  +3.635 * deltaGmu() );
3802 
3803  if (FlagQuadraticTerms) {
3804  //Add contributions that are quadratic in the effective coefficients
3805  mu += 0.0;
3806  }
3807 
3808  } else if (sqrt_s == 0.380) {
3809 
3810  C1 = 0.0062; // Use the same as 350 GeV
3811 
3812  mu +=
3813  +121001. * CiHbox / LambdaNP2
3814  -237126. * CiHL3_11 / LambdaNP2
3815  -203726. * CiHD / LambdaNP2
3816  -42070.9 * CiHW / LambdaNP2
3817  -379788. * CiHWB / LambdaNP2
3818  -31352.7 * CiDHW / LambdaNP2
3819  -4.714 * DeltaGF()
3820  -5.044 * deltaMwd6()
3821  ;
3822 
3823  // Add modifications due to small variations of the SM parameters
3824  mu += cHSM * (
3825  +4.192 * deltaMz()
3826  -1.711 * deltaMh()
3827  -0.618 * deltaaMZ()
3828  +3.64 * deltaGmu() );
3829 
3830  if (FlagQuadraticTerms) {
3831  //Add contributions that are quadratic in the effective coefficients
3832  mu += 0.0;
3833  }
3834 
3835  } else if (sqrt_s == 0.500) {
3836 
3837  C1 = 0.0061;
3838 
3839  mu +=
3840  +121063. * CiHbox / LambdaNP2
3841  -295115. * CiHL3_11 / LambdaNP2
3842  -203679. * CiHD / LambdaNP2
3843  -47539.5 * CiHW / LambdaNP2
3844  -379773. * CiHWB / LambdaNP2
3845  -39825.1 * CiDHW / LambdaNP2
3846  -4.715 * DeltaGF()
3847  -4.817 * deltaMwd6()
3848  ;
3849 
3850  // Add modifications due to small variations of the SM parameters
3851  mu += cHSM * (
3852  +4.509 * deltaMz()
3853  -1.178 * deltaMh()
3854  -0.666 * deltaaMZ()
3855  +3.692 * deltaGmu() );
3856 
3857  if (FlagQuadraticTerms) {
3858  //Add contributions that are quadratic in the effective coefficients
3859  mu += 0.0;
3860  }
3861 
3862  } else if (sqrt_s == 1.0) {
3863 
3864  C1 = 0.0059;
3865 
3866  mu +=
3867  +120960. * CiHbox / LambdaNP2
3868  -442647. * CiHL3_11 / LambdaNP2
3869  -203748. * CiHD / LambdaNP2
3870  -49375.4 * CiHW / LambdaNP2
3871  -379685. * CiHWB / LambdaNP2
3872  -63503.9 * CiDHW / LambdaNP2
3873  -4.712 * DeltaGF()
3874  -4.481 * deltaMwd6()
3875  ;
3876 
3877  // Add modifications due to small variations of the SM parameters
3878  mu += cHSM * (
3879  +4.99 * deltaMz()
3880  -0.582 * deltaMh()
3881  -0.734 * deltaaMZ()
3882  +3.765 * deltaGmu() );
3883 
3884  if (FlagQuadraticTerms) {
3885  //Add contributions that are quadratic in the effective coefficients
3886  mu += 0.0;
3887  }
3888 
3889  } else if (sqrt_s == 1.4) {
3890 
3891  C1 = 0.0058;
3892 
3893  mu +=
3894  +121118. * CiHbox / LambdaNP2
3895  -515189. * CiHL3_11 / LambdaNP2
3896  -203684. * CiHD / LambdaNP2
3897  -46619.5 * CiHW / LambdaNP2
3898  -379667. * CiHWB / LambdaNP2
3899  -75747.8 * CiDHW / LambdaNP2
3900  -4.714 * DeltaGF()
3901  -4.391 * deltaMwd6()
3902  ;
3903 
3904  // Add modifications due to small variations of the SM parameters
3905  mu += cHSM * (
3906  +5.13 * deltaMz()
3907  -0.446 * deltaMh()
3908  -0.754 * deltaaMZ()
3909  +3.784 * deltaGmu() );
3910 
3911  if (FlagQuadraticTerms) {
3912  //Add contributions that are quadratic in the effective coefficients
3913  mu += 0.0;
3914  }
3915 
3916  } else if (sqrt_s == 1.5) {
3917 
3918  C1 = 0.0058;// Use the same as 1400 GeV
3919 
3920  mu +=
3921  +121200. * CiHbox / LambdaNP2
3922  -530152. * CiHL3_11 / LambdaNP2
3923  -203649. * CiHD / LambdaNP2
3924  -45921.3 * CiHW / LambdaNP2
3925  -379591. * CiHWB / LambdaNP2
3926  -78241.3 * CiDHW / LambdaNP2
3927  -4.715 * DeltaGF()
3928  -4.38 * deltaMwd6()
3929  ;
3930 
3931  // Add modifications due to small variations of the SM parameters
3932  mu += cHSM * (
3933  +5.154 * deltaMz()
3934  -0.424 * deltaMh()
3935  -0.757 * deltaaMZ()
3936  +3.786 * deltaGmu() );
3937 
3938  if (FlagQuadraticTerms) {
3939  //Add contributions that are quadratic in the effective coefficients
3940  mu += 0.0;
3941  }
3942 
3943  } else if (sqrt_s == 3.0) {
3944 
3945  C1 = 0.0057;
3946 
3947  mu +=
3948  +121321. * CiHbox / LambdaNP2
3949  -684382. * CiHL3_11 / LambdaNP2
3950  -203585. * CiHD / LambdaNP2
3951  -38239. * CiHW / LambdaNP2
3952  -379518. * CiHWB / LambdaNP2
3953  -104465. * CiDHW / LambdaNP2
3954  -4.714 * DeltaGF()
3955  -4.258 * deltaMwd6()
3956  ;
3957 
3958  // Add modifications due to small variations of the SM parameters
3959  mu += cHSM * (
3960  +5.331 * deltaMz()
3961  -0.279 * deltaMh()
3962  -0.785 * deltaaMZ()
3963  +3.81 * deltaGmu() );
3964 
3965  if (FlagQuadraticTerms) {
3966  //Add contributions that are quadratic in the effective coefficients
3967  mu += 0.0;
3968  }
3969 
3970  } else
3971  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeWBF()");
3972 
3973  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
3974  mu += eeeWBFint + eeeWBFpar;
3975 
3976 // Linear contribution from Higgs self-coupling
3977  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
3978 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
3980 
3981  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
3982 
3983  return mu;
3984 }

◆ mueeWBFPol()

double NPSMEFTd6::mueeWBFPol ( const double  sqrt_s,
const double  Pol_em,
const double  Pol_ep 
) const
virtual

The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively
Returns
\(\mu_{eeWBF}\)

Reimplemented from NPbase.

Definition at line 3987 of file NPSMEFTd6.cpp.

3988 {
3989 
3990 // Pure WBF, hence only initiated by LH fermions. No difference between polarizations at the linear level.
3991 // Expand like other functions when quadratic terms are included
3992 
3993  return mueeWBF(sqrt_s);
3994 }

◆ mueeWW()

double NPSMEFTd6::mueeWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{eeWW}\) between the \( e^{+}e^{-}\to W^{+}W^{-} \) production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{eeWW}\)

Reimplemented from NPbase.

Definition at line 13915 of file NPSMEFTd6.cpp.

13916 {
13917  double mu = 1.0;
13918 
13919  if (sqrt_s == 0.161) {
13920 
13921  mu +=
13922  -127.685 * CiHL1_11 / LambdaNP2
13923  -175.567 * CiHe_11 / LambdaNP2
13924  +242506. * CiHL3_11 / LambdaNP2
13925  -86570.7 * CiHD / LambdaNP2
13926  -189772. * CiHWB / LambdaNP2
13927  +12.769 * CiDHB / LambdaNP2
13928  +6.384 * CiDHW / LambdaNP2
13929  +0. * CiW / LambdaNP2
13930  -2.858 * DeltaGF()
13931  -70.01 * deltaMwd6();
13932 
13933  // Add modifications due to small variations of the SM parameters
13934  mu += cHSM * ( -13.134 * deltaMz()
13935  +0. * deltaaMZ()
13936  +18.795 * deltaGmu() );
13937 
13938  if (FlagQuadraticTerms) {
13939  //Add contributions that are quadratic in the effective coefficients
13940  mu += 0.0;
13941  }
13942 
13943  } else if (sqrt_s == 0.240) {
13944 
13945  mu +=
13946  -26882.4 * CiHL1_11 / LambdaNP2
13947  -17485.4 * CiHe_11 / LambdaNP2
13948  +267456. * CiHL3_11 / LambdaNP2
13949  -83799.2 * CiHD / LambdaNP2
13950  -168074. * CiHWB / LambdaNP2
13951  +3199.72 * CiDHB / LambdaNP2
13952  +3401.93 * CiDHW / LambdaNP2
13953  +6649.22 * CiW / LambdaNP2
13954  -2.812 * DeltaGF()
13955  -0.993 * deltaMwd6();
13956 
13957  // Add modifications due to small variations of the SM parameters
13958  mu += cHSM * ( +4.101 * deltaMz()
13959  -0.584 * deltaaMZ()
13960  +2.688 * deltaGmu() );
13961 
13962  if (FlagQuadraticTerms) {
13963  //Add contributions that are quadratic in the effective coefficients
13964  mu += 0.0;
13965  }
13966 
13967  } else if (sqrt_s == 0.250) {
13968 
13969  mu +=
13970  -29442.7 * CiHL1_11 / LambdaNP2
13971  -18494.5 * CiHe_11 / LambdaNP2
13972  +269747. * CiHL3_11 / LambdaNP2
13973  -83750.9 * CiHD / LambdaNP2
13974  -167811. * CiHWB / LambdaNP2
13975  +3401.99 * CiDHB / LambdaNP2
13976  +3624.67 * CiDHW / LambdaNP2
13977  +7249.33 * CiW / LambdaNP2
13978  -2.812 * DeltaGF()
13979  -0.959 * deltaMwd6();
13980 
13981  // Add modifications due to small variations of the SM parameters
13982  mu += cHSM * ( +4.184 * deltaMz()
13983  -0.585 * deltaaMZ()
13984  +2.709 * deltaGmu() );
13985 
13986  if (FlagQuadraticTerms) {
13987  //Add contributions that are quadratic in the effective coefficients
13988  mu += 0.0;
13989  }
13990 
13991  } else if (sqrt_s == 0.350) {
13992 
13993  mu +=
13994  -47552.4 * CiHL1_11 / LambdaNP2
13995  -23798.8 * CiHe_11 / LambdaNP2
13996  +289379. * CiHL3_11 / LambdaNP2
13997  -83905.3 * CiHD / LambdaNP2
13998  -168326. * CiHWB / LambdaNP2
13999  +5979.05 * CiDHB / LambdaNP2
14000  +6520.95 * CiDHW / LambdaNP2
14001  +10476.9 * CiW / LambdaNP2
14002  -2.832 * DeltaGF()
14003  -0.781 * deltaMwd6();
14004 
14005  // Add modifications due to small variations of the SM parameters
14006  mu += cHSM * ( +4.516 * deltaMz()
14007  -0.659 * deltaaMZ()
14008  +2.768 * deltaGmu());
14009 
14010  if (FlagQuadraticTerms) {
14011  //Add contributions that are quadratic in the effective coefficients
14012  mu += 0.0;
14013  }
14014 
14015  } else if (sqrt_s == 0.365) {
14016 
14017  mu +=
14018  -49800.4 * CiHL1_11 / LambdaNP2
14019  -24520.1 * CiHe_11 / LambdaNP2
14020  +290743. * CiHL3_11 / LambdaNP2
14021  -84033.5 * CiHD / LambdaNP2
14022  -168466. * CiHWB / LambdaNP2
14023  +6310.59 * CiDHB / LambdaNP2
14024  +6842.81 * CiDHW / LambdaNP2
14025  +10606.3 * CiW / LambdaNP2
14026  -2.828 * DeltaGF()
14027  -0.775 * deltaMwd6();
14028 
14029  // Add modifications due to small variations of the SM parameters
14030  mu += cHSM * ( +4.533 * deltaMz()
14031  -0.661 * deltaaMZ()
14032  +2.789 * deltaGmu() );
14033 
14034  if (FlagQuadraticTerms) {
14035  //Add contributions that are quadratic in the effective coefficients
14036  mu += 0.0;
14037  }
14038 
14039  } else if (sqrt_s == 0.500) {
14040 
14041  mu +=
14042  -68234.1 * CiHL1_11 / LambdaNP2
14043  -31290. * CiHe_11 / LambdaNP2
14044  +309504. * CiHL3_11 / LambdaNP2
14045  -84926.8 * CiHD / LambdaNP2
14046  -171658. * CiHWB / LambdaNP2
14047  +9325.19 * CiDHB / LambdaNP2
14048  +10009.9 * CiDHW / LambdaNP2
14049  +10896.4 * CiW / LambdaNP2
14050  -2.84 * DeltaGF()
14051  -0.705 * deltaMwd6();
14052 
14053  // Add modifications due to small variations of the SM parameters
14054  mu += cHSM * ( +4.7 * deltaMz()
14055  -0.683 * deltaaMZ()
14056  +2.799 * deltaGmu() );
14057 
14058  if (FlagQuadraticTerms) {
14059  //Add contributions that are quadratic in the effective coefficients
14060  mu += 0.0;
14061  }
14062 
14063  } else
14064  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeWW()");
14065 
14066  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
14067 
14068  return mu;
14069 }

◆ mueeWWPol()

double NPSMEFTd6::mueeWWPol ( const double  sqrt_s,
const double  Pol_em,
const double  Pol_ep 
) const
virtual

The ratio \(\mu_{eeWW}\) between the \( e^{+}e^{-}\to W^{+}W^{-} \) production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively
Returns
\(\mu_{eeWW}\)

Reimplemented from NPbase.

Definition at line 14072 of file NPSMEFTd6.cpp.

14073 {
14074  double mu = 1.0;
14075 
14076  if (sqrt_s == 0.240) {
14077 
14078  if (Pol_em == 80. && Pol_ep == -30.){
14079  mu +=
14080  -23395. * CiHL1_11 / LambdaNP2
14081  -261092. * CiHe_11 / LambdaNP2
14082  +231526. * CiHL3_11 / LambdaNP2
14083  -72645.8 * CiHD / LambdaNP2
14084  -25084.5 * CiHWB / LambdaNP2
14085  +27060.4 * CiDHB / LambdaNP2
14086  -7822.83 * CiDHW / LambdaNP2
14087  -587.63 * CiW / LambdaNP2
14088  -2.437 * DeltaGF()
14089  -1.554 * deltaMwd6();
14090 
14091  // Add modifications due to small variations of the SM parameters
14092  mu += cHSM * ( +3.226 * deltaMz()
14093  -0.083 * deltaaMZ()
14094  +2.189 * deltaGmu() );
14095 
14096  } else if (Pol_em == -80. && Pol_ep == 30.){
14097  mu +=
14098  -27334.5 * CiHL1_11 / LambdaNP2
14099  -564.392 * CiHe_11 / LambdaNP2
14100  +269600. * CiHL3_11 / LambdaNP2
14101  -84684.5 * CiHD / LambdaNP2
14102  -178168. * CiHWB / LambdaNP2
14103  +1539.25 * CiDHB / LambdaNP2
14104  +4130.32 * CiDHW / LambdaNP2
14105  +7121.6 * CiW / LambdaNP2
14106  -2.838 * DeltaGF()
14107  -0.949 * deltaMwd6();
14108 
14109  // Add modifications due to small variations of the SM parameters
14110  mu += cHSM * ( +4.156 * deltaMz()
14111  -0.607 * deltaaMZ()
14112  +2.724 * deltaGmu() );
14113 
14114  } else {
14115  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeWWPol()");
14116  }
14117 
14118  } else if (sqrt_s == 0.250) {
14119 
14120  if (Pol_em == 80. && Pol_ep == -30.){
14121  mu +=
14122  -25554.9 * CiHL1_11 / LambdaNP2
14123  -274633. * CiHe_11 / LambdaNP2
14124  +234621. * CiHL3_11 / LambdaNP2
14125  -72498.3 * CiHD / LambdaNP2
14126  -23308.5 * CiHWB / LambdaNP2
14127  +29321.9 * CiDHB / LambdaNP2
14128  -7518.62 * CiDHW / LambdaNP2
14129  +314.876 * CiW / LambdaNP2
14130  -2.444 * DeltaGF()
14131  -1.448 * deltaMwd6();
14132 
14133  // Add modifications due to small variations of the SM parameters
14134  mu += cHSM * ( +3.37 * deltaMz()
14135  -0.119 * deltaaMZ()
14136  +2.223 * deltaGmu() );
14137 
14138  } else if (Pol_em == -80. && Pol_ep == 30.){
14139  mu +=
14140  -29714.6 * CiHL1_11 / LambdaNP2
14141  -693.518 * CiHe_11 / LambdaNP2
14142  +271032. * CiHL3_11 / LambdaNP2
14143  -84929.3 * CiHD / LambdaNP2
14144  -177727. * CiHWB / LambdaNP2
14145  +1648.44 * CiDHB / LambdaNP2
14146  +4443.85 * CiDHW / LambdaNP2
14147  +7778.07 * CiW / LambdaNP2
14148  -2.829 * DeltaGF()
14149  -0.914 * deltaMwd6();
14150 
14151  // Add modifications due to small variations of the SM parameters
14152  mu += cHSM * ( +4.233 * deltaMz()
14153  -0.62 * deltaaMZ()
14154  +2.73 * deltaGmu() );
14155 
14156  } else if (Pol_em == 80. && Pol_ep == 0.){
14157  mu +=
14158  -27418.7 * CiHL1_11 / LambdaNP2
14159  -157891. * CiHe_11 / LambdaNP2
14160  +250086. * CiHL3_11 / LambdaNP2
14161  -77904.2 * CiHD / LambdaNP2
14162  -89451.9 * CiHWB / LambdaNP2
14163  +17499.7 * CiDHB / LambdaNP2
14164  -2499.14 * CiDHW / LambdaNP2
14165  +3435.6 * CiW / LambdaNP2
14166  -2.607 * DeltaGF()
14167  -1.242 * deltaMwd6();
14168 
14169  // Add modifications due to small variations of the SM parameters
14170  mu += cHSM * ( +3.759 * deltaMz()
14171  -0.343 * deltaaMZ()
14172  +2.459 * deltaGmu() );
14173 
14174  } else if (Pol_em == -80. && Pol_ep == 0.){
14175  mu +=
14176  -29686. * CiHL1_11 / LambdaNP2
14177  -1698.32 * CiHe_11 / LambdaNP2
14178  +271004. * CiHL3_11 / LambdaNP2
14179  -84881.5 * CiHD / LambdaNP2
14180  -177249. * CiHWB / LambdaNP2
14181  +1732.98 * CiDHB / LambdaNP2
14182  +4380.98 * CiDHW / LambdaNP2
14183  +7742.96 * CiW / LambdaNP2
14184  -2.828 * DeltaGF()
14185  -0.915 * deltaMwd6();
14186 
14187  // Add modifications due to small variations of the SM parameters
14188  mu += cHSM * ( +4.244 * deltaMz()
14189  -0.624 * deltaaMZ()
14190  +2.729 * deltaGmu() );
14191 
14192  } else {
14193  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeWWPol()");
14194  }
14195 
14196  } else if (sqrt_s == 0.350) {
14197 
14198  if (Pol_em == 80. && Pol_ep == -30.){
14199  mu +=
14200  -43312.4 * CiHL1_11 / LambdaNP2
14201  -370403. * CiHe_11 / LambdaNP2
14202  +262809. * CiHL3_11 / LambdaNP2
14203  -76119.5 * CiHD / LambdaNP2
14204  -35565.5 * CiHWB / LambdaNP2
14205  +48488.8 * CiDHB / LambdaNP2
14206  -4519.05 * CiDHW / LambdaNP2
14207  +6279.71 * CiW / LambdaNP2
14208  -2.571 * DeltaGF()
14209  -1.059 * deltaMwd6();
14210 
14211  // Add modifications due to small variations of the SM parameters
14212  mu += cHSM * ( +4.035 * deltaMz()
14213  -0.336 * deltaaMZ()
14214  +2.471 * deltaGmu() );
14215 
14216  } else if (Pol_em == -80. && Pol_ep == 30.){
14217  mu +=
14218  -47925. * CiHL1_11 / LambdaNP2
14219  -912.302 * CiHe_11 / LambdaNP2
14220  +290384. * CiHL3_11 / LambdaNP2
14221  -84475.3 * CiHD / LambdaNP2
14222  -177142. * CiHWB / LambdaNP2
14223  +3105.71 * CiDHB / LambdaNP2
14224  +7205.25 * CiDHW / LambdaNP2
14225  +10660.4 * CiW / LambdaNP2
14226  -2.841 * DeltaGF()
14227  -0.773 * deltaMwd6();
14228 
14229  // Add modifications due to small variations of the SM parameters
14230  mu += cHSM * ( +4.542 * deltaMz()
14231  -0.672 * deltaaMZ()
14232  +2.797 * deltaGmu() );
14233 
14234  } else if (Pol_em == 80. && Pol_ep == 0.){
14235  mu +=
14236  -45448.7 * CiHL1_11 / LambdaNP2
14237  -208484. * CiHe_11 / LambdaNP2
14238  +274583. * CiHL3_11 / LambdaNP2
14239  -80024.1 * CiHD / LambdaNP2
14240  -97902.7 * CiHWB / LambdaNP2
14241  +28562.8 * CiDHB / LambdaNP2
14242  +575.898 * CiDHW / LambdaNP2
14243  +8122.74 * CiW / LambdaNP2
14244  -2.687 * DeltaGF()
14245  -0.928 * deltaMwd6();
14246 
14247  // Add modifications due to small variations of the SM parameters
14248  mu += cHSM * ( +4.257 * deltaMz()
14249  -0.496 * deltaaMZ()
14250  +2.607 * deltaGmu() );
14251 
14252  } else if (Pol_em == -80. && Pol_ep == 0.){
14253  mu +=
14254  -47903.7 * CiHL1_11 / LambdaNP2
14255  -2144.19 * CiHe_11 / LambdaNP2
14256  +290349. * CiHL3_11 / LambdaNP2
14257  -84405.4 * CiHD / LambdaNP2
14258  -176530. * CiHWB / LambdaNP2
14259  +3309.62 * CiDHB / LambdaNP2
14260  +7174.21 * CiDHW / LambdaNP2
14261  +10675.5 * CiW / LambdaNP2
14262  -2.84 * DeltaGF()
14263  -0.777 * deltaMwd6();
14264 
14265  // Add modifications due to small variations of the SM parameters
14266  mu += cHSM * ( +4.543 * deltaMz()
14267  -0.674 * deltaaMZ()
14268  +2.798 * deltaGmu() );
14269 
14270  } else {
14271  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeWWPol()");
14272  }
14273 
14274  } else if (sqrt_s == 0.365) {
14275 
14276  if (Pol_em == 80. && Pol_ep == -30.){
14277  mu +=
14278  -45618.2 * CiHL1_11 / LambdaNP2
14279  -382668. * CiHe_11 / LambdaNP2
14280  +265703. * CiHL3_11 / LambdaNP2
14281  -77085.4 * CiHD / LambdaNP2
14282  -38791. * CiHWB / LambdaNP2
14283  +51079.9 * CiDHB / LambdaNP2
14284  -3972.2 * CiDHW / LambdaNP2
14285  +6727.91 * CiW / LambdaNP2
14286  -2.582 * DeltaGF()
14287  -1.04 * deltaMwd6();
14288 
14289  // Add modifications due to small variations of the SM parameters
14290  mu += cHSM * ( +4.09 * deltaMz()
14291  -0.349 * deltaaMZ()
14292  +2.483 * deltaGmu() );
14293 
14294  } else if (Pol_em == -80. && Pol_ep == 30.){
14295  mu +=
14296  -50230.7 * CiHL1_11 / LambdaNP2
14297  -1000.53 * CiHe_11 / LambdaNP2
14298  +291951. * CiHL3_11 / LambdaNP2
14299  -84657.2 * CiHD / LambdaNP2
14300  -177196. * CiHWB / LambdaNP2
14301  +3348.72 * CiDHB / LambdaNP2
14302  +7579.53 * CiDHW / LambdaNP2
14303  +10879.2 * CiW / LambdaNP2
14304  -2.84 * DeltaGF()
14305  -0.753 * deltaMwd6();
14306 
14307  // Add modifications due to small variations of the SM parameters
14308  mu += cHSM * ( +4.576 * deltaMz()
14309  -0.681 * deltaaMZ()
14310  +2.795 * deltaGmu() );
14311 
14312  } else {
14313  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeWWPol()");
14314  }
14315 
14316  } else if (sqrt_s == 0.380) {
14317 
14318  if (Pol_em == 80. && Pol_ep == 0.){
14319  mu +=
14320  -49806.5 * CiHL1_11 / LambdaNP2
14321  -221155. * CiHe_11 / LambdaNP2
14322  +280445. * CiHL3_11 / LambdaNP2
14323  -80550.4 * CiHD / LambdaNP2
14324  -101476. * CiHWB / LambdaNP2
14325  +31723.3 * CiDHB / LambdaNP2
14326  +1672.16 * CiDHW / LambdaNP2
14327  +8838.57 * CiW / LambdaNP2
14328  -2.707 * DeltaGF()
14329  -0.891 * deltaMwd6();
14330 
14331  // Add modifications due to small variations of the SM parameters
14332  mu += cHSM * ( +4.331 * deltaMz()
14333  -0.503 * deltaaMZ()
14334  +2.64 * deltaGmu() );
14335 
14336  } else if (Pol_em == -80. && Pol_ep == 0.){
14337  mu +=
14338  -52386.5 * CiHL1_11 / LambdaNP2
14339  -2537.08 * CiHe_11 / LambdaNP2
14340  +294134. * CiHL3_11 / LambdaNP2
14341  -84922.5 * CiHD / LambdaNP2
14342  -176871. * CiHWB / LambdaNP2
14343  +3635.55 * CiDHB / LambdaNP2
14344  +7973.68 * CiDHW / LambdaNP2
14345  +10984.7 * CiW / LambdaNP2
14346  -2.838 * DeltaGF()
14347  -0.753 * deltaMwd6();
14348 
14349  // Add modifications due to small variations of the SM parameters
14350  mu += cHSM * ( +4.589 * deltaMz()
14351  -0.68 * deltaaMZ()
14352  +2.81 * deltaGmu() );
14353 
14354  } else {
14355  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeWWPol()");
14356  }
14357 
14358  } else if (sqrt_s == 0.500) {
14359 
14360  if (Pol_em == 80. && Pol_ep == -30.){
14361  mu +=
14362  -64264.6 * CiHL1_11 / LambdaNP2
14363  -495727. * CiHe_11 / LambdaNP2
14364  +289682. * CiHL3_11 / LambdaNP2
14365  -80108.8 * CiHD / LambdaNP2
14366  -61678. * CiHWB / LambdaNP2
14367  +75403.3 * CiDHB / LambdaNP2
14368  +458.146 * CiDHW / LambdaNP2
14369  +8723.87 * CiW / LambdaNP2
14370  -2.664 * DeltaGF()
14371  -0.849 * deltaMwd6();
14372 
14373  // Add modifications due to small variations of the SM parameters
14374  mu += cHSM * ( +4.362 * deltaMz()
14375  -0.496 * deltaaMZ()
14376  +2.591 * deltaGmu() );
14377 
14378  } else if (Pol_em == -80. && Pol_ep == 30.){
14379  mu +=
14380  -68310.7 * CiHL1_11 / LambdaNP2
14381  -1341.22 * CiHe_11 / LambdaNP2
14382  +311528. * CiHL3_11 / LambdaNP2
14383  -84984.5 * CiHD / LambdaNP2
14384  -178260. * CiHWB / LambdaNP2
14385  +5206.37 * CiDHB / LambdaNP2
14386  +10705.4 * CiDHW / LambdaNP2
14387  +11071.1 * CiW / LambdaNP2
14388  -2.855 * DeltaGF()
14389  -0.671 * deltaMwd6();
14390 
14391  // Add modifications due to small variations of the SM parameters
14392  mu += cHSM * ( +4.728 * deltaMz()
14393  -0.698 * deltaaMZ()
14394  +2.817 * deltaGmu() );
14395 
14396  } else if (Pol_em == 80. && Pol_ep == 0.){
14397  mu +=
14398  -66178. * CiHL1_11 / LambdaNP2
14399  -274919. * CiHe_11 / LambdaNP2
14400  +299745. * CiHL3_11 / LambdaNP2
14401  -82524.6 * CiHD / LambdaNP2
14402  -113979. * CiHWB / LambdaNP2
14403  +43898.4 * CiDHB / LambdaNP2
14404  +5024.43 * CiDHW / LambdaNP2
14405  +9759.79 * CiW / LambdaNP2
14406  -2.752 * DeltaGF()
14407  -0.778 * deltaMwd6();
14408 
14409  // Add modifications due to small variations of the SM parameters
14410  mu += cHSM * ( +4.515 * deltaMz()
14411  -0.602 * deltaaMZ()
14412  +2.695 * deltaGmu() );
14413 
14414  } else if (Pol_em == -80. && Pol_ep == 0.){
14415  mu +=
14416  -68435.6 * CiHL1_11 / LambdaNP2
14417  -3089.11 * CiHe_11 / LambdaNP2
14418  +310020. * CiHL3_11 / LambdaNP2
14419  -85227.7 * CiHD / LambdaNP2
14420  -178139. * CiHWB / LambdaNP2
14421  +5322.77 * CiDHB / LambdaNP2
14422  +10598. * CiDHW / LambdaNP2
14423  +11009.9 * CiW / LambdaNP2
14424  -2.846 * DeltaGF()
14425  -0.681 * deltaMwd6();
14426 
14427  // Add modifications due to small variations of the SM parameters
14428  mu += cHSM * ( +4.725 * deltaMz()
14429  -0.695 * deltaaMZ()
14430  +2.828 * deltaGmu() );
14431 
14432  } else {
14433  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeWWPol()");
14434  }
14435 
14436  } else if (sqrt_s == 1.0) {
14437 
14438  if (Pol_em == 80. && Pol_ep == -20.){
14439  mu +=
14440  -145951. * CiHL1_11 / LambdaNP2
14441  -885593. * CiHe_11 / LambdaNP2
14442  +383080. * CiHL3_11 / LambdaNP2
14443  -83628.6 * CiHD / LambdaNP2
14444  -114732. * CiHWB / LambdaNP2
14445  +159832. * CiDHB / LambdaNP2
14446  +17735.5 * CiDHW / LambdaNP2
14447  +8916.37 * CiW / LambdaNP2
14448  -2.787 * DeltaGF()
14449  -0.57 * deltaMwd6() ;
14450 
14451  // Add modifications due to small variations of the SM parameters
14452  mu += cHSM * ( +4.793 * deltaMz()
14453  -0.653 * deltaaMZ()
14454  +2.677 * deltaGmu() );
14455 
14456  } else if (Pol_em == -80. && Pol_ep == 20.){
14457  mu +=
14458  -150086. * CiHL1_11 / LambdaNP2
14459  -4395.1 * CiHe_11 / LambdaNP2
14460  +394641. * CiHL3_11 / LambdaNP2
14461  -85925.1 * CiHD / LambdaNP2
14462  -181046. * CiHWB / LambdaNP2
14463  +13333.6 * CiDHB / LambdaNP2
14464  +23871.2 * CiDHW / LambdaNP2
14465  +9450.35 * CiW / LambdaNP2
14466  -2.871 * DeltaGF()
14467  -0.492 * deltaMwd6() ;
14468 
14469  // Add modifications due to small variations of the SM parameters
14470  mu += cHSM * ( +5.001 * deltaMz()
14471  -0.752 * deltaaMZ()
14472  +2.79 * deltaGmu() );
14473 
14474  } else {
14475  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeWWPol()");
14476  }
14477 
14478  } else if (sqrt_s == 1.5) {
14479 
14480  if (Pol_em == 80. && Pol_ep == 0.){
14481  mu +=
14482  -261040. * CiHL1_11 / LambdaNP2
14483  -1059495. * CiHe_11 / LambdaNP2
14484  +500666. * CiHL3_11 / LambdaNP2
14485  -84992.3 * CiHD / LambdaNP2
14486  -144925. * CiHWB / LambdaNP2
14487  +205215. * CiDHB / LambdaNP2
14488  +38777.5 * CiDHW / LambdaNP2
14489  +7857.84 * CiW / LambdaNP2
14490  -2.817 * DeltaGF()
14491  -0.471 * deltaMwd6();
14492 
14493  // Add modifications due to small variations of the SM parameters
14494  mu += cHSM * ( +4.975 * deltaMz()
14495  -0.718 * deltaaMZ()
14496  +2.688 * deltaGmu() );
14497 
14498  } else if (Pol_em == -80. && Pol_ep == 0.){
14499  mu +=
14500  -265008. * CiHL1_11 / LambdaNP2
14501  -13002.4 * CiHe_11 / LambdaNP2
14502  +507924. * CiHL3_11 / LambdaNP2
14503  -86313.9 * CiHD / LambdaNP2
14504  -182113. * CiHWB / LambdaNP2
14505  +24953.6 * CiDHB / LambdaNP2
14506  +42429.8 * CiDHW / LambdaNP2
14507  +8014.86 * CiW / LambdaNP2
14508  -2.857 * DeltaGF()
14509  -0.429 * deltaMwd6();
14510 
14511  // Add modifications due to small variations of the SM parameters
14512  mu += cHSM * ( +5.094 * deltaMz()
14513  -0.768 * deltaaMZ()
14514  +2.739 * deltaGmu() );
14515 
14516  } else {
14517  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeWWPol()");
14518  }
14519 
14520  } else if (sqrt_s == 3.0) {
14521 
14522  if (Pol_em == 80. && Pol_ep == 0.){
14523  mu +=
14524  -776767. * CiHL1_11 / LambdaNP2
14525  -3168410. * CiHe_11 / LambdaNP2
14526  +1016120. * CiHL3_11 / LambdaNP2
14527  -85414.3 * CiHD / LambdaNP2
14528  -155729. * CiHWB / LambdaNP2
14529  +628130. * CiDHB / LambdaNP2
14530  +123368. * CiDHW / LambdaNP2
14531  +6454.34 * CiW / LambdaNP2
14532  -2.831 * DeltaGF()
14533  -0.352 * deltaMwd6();
14534 
14535  // Add modifications due to small variations of the SM parameters
14536  mu += cHSM * ( +5.165 * deltaMz()
14537  -0.755 * deltaaMZ()
14538  +2.77 * deltaGmu() );
14539 
14540  } else if (Pol_em == -80. && Pol_ep == 0.){
14541  mu +=
14542  -785359. * CiHL1_11 / LambdaNP2
14543  -39533. * CiHe_11 / LambdaNP2
14544  +1027322. * CiHL3_11 / LambdaNP2
14545  -86621.7 * CiHD / LambdaNP2
14546  -184516. * CiHWB / LambdaNP2
14547  +75975.5 * CiDHB / LambdaNP2
14548  +127086. * CiDHW / LambdaNP2
14549  +6519.78 * CiW / LambdaNP2
14550  -2.86 * DeltaGF()
14551  -0.328 * deltaMwd6();
14552 
14553  // Add modifications due to small variations of the SM parameters
14554  mu += cHSM * ( +5.246 * deltaMz()
14555  -0.79 * deltaaMZ()
14556  +2.81 * deltaGmu() );
14557 
14558  } else {
14559  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeWWPol()");
14560  }
14561 
14562  } else
14563  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeWWPol()");
14564 
14565  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
14566 
14567  return mu;
14568 }

◆ mueeZBF()

double NPSMEFTd6::mueeZBF ( const double  sqrt_s) const
virtual

The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{eeZBF}\)

Reimplemented from NPbase.

Definition at line 5359 of file NPSMEFTd6.cpp.

5360 {
5361  double mu = 1.0;
5362 
5363  double C1 = 0.0;
5364 
5365  if (sqrt_s == 0.240) {
5366 
5367  C1 = 0.0070;
5368 
5369  mu +=
5370  +121661. * CiHbox / LambdaNP2
5371  +489617. * CiHL1_11 / LambdaNP2
5372  -357163. * CiHe_11 / LambdaNP2
5373  +489617. * CiHL3_11 / LambdaNP2
5374  -39217.8 * CiHD / LambdaNP2
5375  +1525468. * CiHB / LambdaNP2
5376  +378019. * CiHW / LambdaNP2
5377  +215983. * CiHWB / LambdaNP2
5378  -6554.11 * CiDHB / LambdaNP2
5379  +1175.47 * CiDHW / LambdaNP2
5380  -3.161 * DeltaGF()
5381  ;
5382 
5383  // Add modifications due to small variations of the SM parameters
5384  mu += cHSM * ( +0.908 * deltaMz()
5385  -5.799 * deltaMh()
5386  -0.248 * deltaaMZ()
5387  +3.158 * deltaGmu() );
5388 
5389  if (FlagQuadraticTerms) {
5390  //Add contributions that are quadratic in the effective coefficients
5391  mu += 0.0;
5392  }
5393 
5394  } else if (sqrt_s == 0.250) {
5395 
5396  C1 = 0.0070;
5397 
5398  mu +=
5399  +122144. * CiHbox / LambdaNP2
5400  +444406. * CiHL1_11 / LambdaNP2
5401  -315727. * CiHe_11 / LambdaNP2
5402  +444406. * CiHL3_11 / LambdaNP2
5403  -41440.8 * CiHD / LambdaNP2
5404  +1186855. * CiHB / LambdaNP2
5405  +301913. * CiHW / LambdaNP2
5406  +98540.5 * CiHWB / LambdaNP2
5407  -5766.35 * CiDHB / LambdaNP2
5408  +294.724 * CiDHW / LambdaNP2
5409  -3.279 * DeltaGF()
5410  ;
5411 
5412  // Add modifications due to small variations of the SM parameters
5413  mu += cHSM * ( +2.044 * deltaMz()
5414  -4.578 * deltaMh()
5415  -0.341 * deltaaMZ()
5416  +3.283 * deltaGmu() );
5417 
5418  if (FlagQuadraticTerms) {
5419  //Add contributions that are quadratic in the effective coefficients
5420  mu += 0.0;
5421  }
5422 
5423  } else if (sqrt_s == 0.350) {
5424 
5425  C1 = 0.0069;
5426 
5427  mu +=
5428  +121556. * CiHbox / LambdaNP2
5429  +46354.9 * CiHL1_11 / LambdaNP2
5430  -251.929 * CiHe_11 / LambdaNP2
5431  +46354.9 * CiHL3_11 / LambdaNP2
5432  -43426.2 * CiHD / LambdaNP2
5433  +450512. * CiHB / LambdaNP2
5434  +166493. * CiHW / LambdaNP2
5435  -198898. * CiHWB / LambdaNP2
5436  -4408.76 * CiDHB / LambdaNP2
5437  -17005.2 * CiDHW / LambdaNP2
5438  -3.427 * DeltaGF()
5439  ;
5440 
5441  // Add modifications due to small variations of the SM parameters
5442  mu += cHSM * ( +3.845 * deltaMz()
5443  -1.857 * deltaMh()
5444  -0.423 * deltaaMZ()
5445  +3.407 * deltaGmu() );
5446 
5447  if (FlagQuadraticTerms) {
5448  //Add contributions that are quadratic in the effective coefficients
5449  mu += 0.0;
5450  }
5451 
5452  } else if (sqrt_s == 0.365) {
5453 
5454  C1 = 0.0069; // use same as 350 GeV
5455 
5456  mu +=
5457  +121067. * CiHbox / LambdaNP2
5458  +9887.64 * CiHL1_11 / LambdaNP2
5459  +27809. * CiHe_11 / LambdaNP2
5460  +9887.64 * CiHL3_11 / LambdaNP2
5461  -43174.2 * CiHD / LambdaNP2
5462  +417865. * CiHB / LambdaNP2
5463  +154270. * CiHW / LambdaNP2
5464  -201517. * CiHWB / LambdaNP2
5465  -4943.82 * CiDHB / LambdaNP2
5466  -19213.5 * CiDHW / LambdaNP2
5467  -3.423 * DeltaGF()
5468  ;
5469 
5470  // Add modifications due to small variations of the SM parameters
5471  mu += cHSM * ( +3.861 * deltaMz()
5472  -1.736 * deltaMh()
5473  -0.426 * deltaaMZ()
5474  +3.375 * deltaGmu() );
5475 
5476  if (FlagQuadraticTerms) {
5477  //Add contributions that are quadratic in the effective coefficients
5478  mu += 0.0;
5479  }
5480 
5481  } else if (sqrt_s == 0.380) {
5482 
5483  C1 = 0.0069; // use same as 350 GeV
5484 
5485  mu +=
5486  +121214. * CiHbox / LambdaNP2
5487  -22289.7 * CiHL1_11 / LambdaNP2
5488  +52903.2 * CiHe_11 / LambdaNP2
5489  -22289.7 * CiHL3_11 / LambdaNP2
5490  -43137.3 * CiHD / LambdaNP2
5491  +388336. * CiHB / LambdaNP2
5492  +140923. * CiHW / LambdaNP2
5493  -202884. * CiHWB / LambdaNP2
5494  -5363.69 * CiDHB / LambdaNP2
5495  -21404.2 * CiDHW / LambdaNP2
5496  -3.418 * DeltaGF()
5497  ;
5498 
5499  // Add modifications due to small variations of the SM parameters
5500  mu += cHSM * ( +3.887 * deltaMz()
5501  -1.633 * deltaMh()
5502  -0.419 * deltaaMZ()
5503  +3.393 * deltaGmu() );
5504 
5505  if (FlagQuadraticTerms) {
5506  //Add contributions that are quadratic in the effective coefficients
5507  mu += 0.0;
5508  }
5509 
5510  } else if (sqrt_s == 0.500) {
5511 
5512  C1 = 0.0067;
5513 
5514  mu +=
5515  +121453. * CiHbox / LambdaNP2
5516  -185326. * CiHL1_11 / LambdaNP2
5517  +178925. * CiHe_11 / LambdaNP2
5518  -185326. * CiHL3_11 / LambdaNP2
5519  -42051.6 * CiHD / LambdaNP2
5520  +236945. * CiHB / LambdaNP2
5521  +67833.5 * CiHW / LambdaNP2
5522  -178623. * CiHWB / LambdaNP2
5523  -8004.61 * CiDHB / LambdaNP2
5524  -33567.3 * CiDHW / LambdaNP2
5525  -3.416 * DeltaGF()
5526  ;
5527 
5528  // Add modifications due to small variations of the SM parameters
5529  mu += cHSM * ( +3.963 * deltaMz()
5530  -1.143 * deltaMh()
5531  -0.408 * deltaaMZ()
5532  +3.383 * deltaGmu() );
5533 
5534  if (FlagQuadraticTerms) {
5535  //Add contributions that are quadratic in the effective coefficients
5536  mu += 0.0;
5537  }
5538 
5539  } else if (sqrt_s == 1.0) {
5540 
5541  C1 = 0.0065;
5542 
5543  mu +=
5544  +121062. * CiHbox / LambdaNP2
5545  -409543. * CiHL1_11 / LambdaNP2
5546  +356730. * CiHe_11 / LambdaNP2
5547  -409543. * CiHL3_11 / LambdaNP2
5548  -42133.9 * CiHD / LambdaNP2
5549  +69851. * CiHB / LambdaNP2
5550  -14416.8 * CiHW / LambdaNP2
5551  -113198. * CiHWB / LambdaNP2
5552  -18688.4 * CiDHB / LambdaNP2
5553  -61696. * CiDHW / LambdaNP2
5554  -3.405 * DeltaGF()
5555  ;
5556 
5557  // Add modifications due to small variations of the SM parameters
5558  mu += cHSM * ( +4.216 * deltaMz()
5559  -0.546 * deltaMh()
5560  -0.407 * deltaaMZ()
5561  +3.393 * deltaGmu() );
5562 
5563  if (FlagQuadraticTerms) {
5564  //Add contributions that are quadratic in the effective coefficients
5565  mu += 0.0;
5566  }
5567 
5568  } else if (sqrt_s == 1.4) {
5569 
5570  C1 = 0.0065;
5571 
5572  mu +=
5573  +120749. * CiHbox / LambdaNP2
5574  -493617. * CiHL1_11 / LambdaNP2
5575  +426669. * CiHe_11 / LambdaNP2
5576  -493617. * CiHL3_11 / LambdaNP2
5577  -42486.9 * CiHD / LambdaNP2
5578  +34633.1 * CiHB / LambdaNP2
5579  -27609.6 * CiHW / LambdaNP2
5580  -97014.2 * CiHWB / LambdaNP2
5581  -23942.2 * CiDHB / LambdaNP2
5582  -74940.3 * CiDHW / LambdaNP2
5583  -3.405 * DeltaGF()
5584  ;
5585 
5586  // Add modifications due to small variations of the SM parameters
5587  mu += cHSM * ( +4.309 * deltaMz()
5588  -0.422 * deltaMh()
5589  -0.402 * deltaaMZ()
5590  +3.379 * deltaGmu() );
5591 
5592  if (FlagQuadraticTerms) {
5593  //Add contributions that are quadratic in the effective coefficients
5594  mu += 0.0;
5595  }
5596 
5597  } else if (sqrt_s == 1.5) {
5598 
5599  C1 = 0.0065;// Use the same as 1400 GeV
5600 
5601  mu +=
5602  +120587. * CiHbox / LambdaNP2
5603  -510290. * CiHL1_11 / LambdaNP2
5604  +440504. * CiHe_11 / LambdaNP2
5605  -510290. * CiHL3_11 / LambdaNP2
5606  -42529.6 * CiHD / LambdaNP2
5607  +30448.1 * CiHB / LambdaNP2
5608  -30741.2 * CiHW / LambdaNP2
5609  -95903.3 * CiHWB / LambdaNP2
5610  -25074.9 * CiDHB / LambdaNP2
5611  -77634.5 * CiDHW / LambdaNP2
5612  -3.401 * DeltaGF()
5613  ;
5614 
5615  // Add modifications due to small variations of the SM parameters
5616  mu += cHSM * ( +4.326 * deltaMz()
5617  -0.4 * deltaMh()
5618  -0.403 * deltaaMZ()
5619  +3.37 * deltaGmu() );
5620 
5621  if (FlagQuadraticTerms) {
5622  //Add contributions that are quadratic in the effective coefficients
5623  mu += 0.0;
5624  }
5625 
5626  } else if (sqrt_s == 3.0) {
5627 
5628  C1 = 0.0063;
5629 
5630  mu +=
5631  +120474. * CiHbox / LambdaNP2
5632  -677185. * CiHL1_11 / LambdaNP2
5633  +582037. * CiHe_11 / LambdaNP2
5634  -677185. * CiHL3_11 / LambdaNP2
5635  -42541.3 * CiHD / LambdaNP2
5636  +6810.6 * CiHB / LambdaNP2
5637  -32994.5 * CiHW / LambdaNP2
5638  -78012.3 * CiHWB / LambdaNP2
5639  -36250. * CiDHB / LambdaNP2
5640  -105734. * CiDHW / LambdaNP2
5641  -3.405 * DeltaGF()
5642  ;
5643 
5644  // Add modifications due to small variations of the SM parameters
5645  mu += cHSM * ( +4.463 * deltaMz()
5646  -0.265 * deltaMh()
5647  -0.405 * deltaaMZ()
5648  +3.351 * deltaGmu() );
5649 
5650  if (FlagQuadraticTerms) {
5651  //Add contributions that are quadratic in the effective coefficients
5652  mu += 0.0;
5653  }
5654 
5655  } else
5656  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBF()");
5657 
5658  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
5659  //(Assume similar to WBF.)
5660  mu += eeeWBFint + eeeWBFpar;
5661 
5662 // Linear contribution from Higgs self-coupling
5663  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
5664 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
5666 
5667  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
5668 
5669  return mu;
5670 }

◆ mueeZBFPol()

double NPSMEFTd6::mueeZBFPol ( const double  sqrt_s,
const double  Pol_em,
const double  Pol_ep 
) const
virtual

The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively
Returns
\(\mu_{eeZBF}\)

Reimplemented from NPbase.

Definition at line 5673 of file NPSMEFTd6.cpp.

5674 {
5675  double mu = 1.0;
5676 
5677  double C1 = 0.0;
5678 
5679  if (sqrt_s == 0.240) {
5680 
5681  C1 = 0.0070;
5682 
5683  if (Pol_em == 80. && Pol_ep == -30.){
5684  mu +=
5685  +121531. * CiHbox / LambdaNP2
5686  +58943.5 * CiHL1_11 / LambdaNP2
5687  -939512. * CiHe_11 / LambdaNP2
5688  +58943.5 * CiHL3_11 / LambdaNP2
5689  +77442.6 * CiHD / LambdaNP2
5690  +2082256. * CiHB / LambdaNP2
5691  +108043. * CiHW / LambdaNP2
5692  +1362693. * CiHWB / LambdaNP2
5693  +40385. * CiDHB / LambdaNP2
5694  -21886. * CiDHW / LambdaNP2
5695  +0.563 * DeltaGF()
5696  ;
5697 
5698  // Add modifications due to small variations of the SM parameters
5699  mu += cHSM * ( -6.582 * deltaMz()
5700  -5.732 * deltaMh()
5701  +3.573 * deltaaMZ()
5702  -0.708 * deltaGmu() );
5703 
5704  } else if (Pol_em == -80. && Pol_ep == 30.){
5705  mu +=
5706  +122065. * CiHbox / LambdaNP2
5707  +905327. * CiHL1_11 / LambdaNP2
5708  -55689. * CiHe_11 / LambdaNP2
5709  +905327. * CiHL3_11 / LambdaNP2
5710  -124548. * CiHD / LambdaNP2
5711  +905057. * CiHB / LambdaNP2
5712  +540185. * CiHW / LambdaNP2
5713  -329708. * CiHWB / LambdaNP2
5714  -37296.9 * CiDHB / LambdaNP2
5715  +20497.1 * CiDHW / LambdaNP2
5716  -5.854 * DeltaGF()
5717  ;
5718 
5719  // Add modifications due to small variations of the SM parameters
5720  mu += cHSM * ( +6.473 * deltaMz()
5721  -5.971 * deltaMh()
5722  -3.019 * deltaaMZ()
5723  +5.959 * deltaGmu() );
5724 
5725  } else if (Pol_em == 80. && Pol_ep == 0.){
5726  mu +=
5727  +121947. * CiHbox / LambdaNP2
5728  +88774.4 * CiHL1_11 / LambdaNP2
5729  -753269. * CiHe_11 / LambdaNP2
5730  +88774.4 * CiHL3_11 / LambdaNP2
5731  +54593.2 * CiHD / LambdaNP2
5732  +2101955. * CiHB / LambdaNP2
5733  +182237. * CiHW / LambdaNP2
5734  +972861. * CiHWB / LambdaNP2
5735  +29346.2 * CiDHB / LambdaNP2
5736  -18562.1 * CiDHW / LambdaNP2
5737  -0.206 * DeltaGF()
5738  ;
5739 
5740  // Add modifications due to small variations of the SM parameters
5741  mu += cHSM * ( -5.131 * deltaMz()
5742  -5.658 * deltaMh()
5743  +2.794 * deltaaMZ()
5744  +0.082 * deltaGmu() );
5745 
5746  } else if (Pol_em == -80. && Pol_ep == 0.){
5747  mu +=
5748  +122265. * CiHbox / LambdaNP2
5749  +785643. * CiHL1_11 / LambdaNP2
5750  -66907.6 * CiHe_11 / LambdaNP2
5751  +785643. * CiHL3_11 / LambdaNP2
5752  -107673. * CiHD / LambdaNP2
5753  +1115316. * CiHB / LambdaNP2
5754  +521873. * CiHW / LambdaNP2
5755  -331727. * CiHWB / LambdaNP2
5756  -32442.4 * CiDHB / LambdaNP2
5757  +15348.7 * CiDHW / LambdaNP2
5758  -5.334 * DeltaGF()
5759  ;
5760 
5761  // Add modifications due to small variations of the SM parameters
5762  mu += cHSM * ( +5.367 * deltaMz()
5763  -5.87 * deltaMh()
5764  -2.491 * deltaaMZ()
5765  +5.409 * deltaGmu() );
5766 
5767  } else {
5768  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
5769  }
5770 
5771  } else if (sqrt_s == 0.250) {
5772 
5773  C1 = 0.0070;
5774 
5775  if (Pol_em == 80. && Pol_ep == -30.){
5776  mu +=
5777  +121054. * CiHbox / LambdaNP2
5778  +51113. * CiHL1_11 / LambdaNP2
5779  -851357. * CiHe_11 / LambdaNP2
5780  +51113. * CiHL3_11 / LambdaNP2
5781  +76762.9 * CiHD / LambdaNP2
5782  +1629614. * CiHB / LambdaNP2
5783  +72741.6 * CiHW / LambdaNP2
5784  +1130834. * CiHWB / LambdaNP2
5785  +34381.7 * CiDHB / LambdaNP2
5786  -19876.5 * CiDHW / LambdaNP2
5787  +0.563 * DeltaGF()
5788  ;
5789 
5790  // Add modifications due to small variations of the SM parameters
5791  mu += cHSM * ( -5.658 * deltaMz()
5792  -4.485 * deltaMh()
5793  +3.577 * deltaaMZ()
5794  -0.638 * deltaGmu() );
5795 
5796  } else if (Pol_em == -80. && Pol_ep == 30.){
5797  mu +=
5798  +121471. * CiHbox / LambdaNP2
5799  +824294. * CiHL1_11 / LambdaNP2
5800  -45066.5 * CiHe_11 / LambdaNP2
5801  +824294. * CiHL3_11 / LambdaNP2
5802  -128864. * CiHD / LambdaNP2
5803  +644513. * CiHB / LambdaNP2
5804  +425051. * CiHW / LambdaNP2
5805  -383720. * CiHWB / LambdaNP2
5806  -32434.3 * CiDHB / LambdaNP2
5807  +15329.4 * CiDHW / LambdaNP2
5808  -6.022 * DeltaGF()
5809  ;
5810 
5811  // Add modifications due to small variations of the SM parameters
5812  mu += cHSM * ( +7.852 * deltaMz()
5813  -4.536 * deltaMh()
5814  -3.165 * deltaaMZ()
5815  +6.136 * deltaGmu() );
5816 
5817  } else if (Pol_em == 80. && Pol_ep == 0.){
5818  mu +=
5819  +121494. * CiHbox / LambdaNP2
5820  +77372.1 * CiHL1_11 / LambdaNP2
5821  -676199. * CiHe_11 / LambdaNP2
5822  +77372.1 * CiHL3_11 / LambdaNP2
5823  +53294.7 * CiHD / LambdaNP2
5824  +1668830. * CiHB / LambdaNP2
5825  +145010. * CiHW / LambdaNP2
5826  +772902. * CiHWB / LambdaNP2
5827  +23910.6 * CiDHB / LambdaNP2
5828  -16890.6 * CiDHW / LambdaNP2
5829  -0.226 * DeltaGF()
5830  ;
5831 
5832  // Add modifications due to small variations of the SM parameters
5833  mu += cHSM * ( -4.183 * deltaMz()
5834  -4.557 * deltaMh()
5835  +2.773 * deltaaMZ()
5836  +0.148 * deltaGmu() );
5837 
5838  } else if (Pol_em == -80. && Pol_ep == 0.){
5839  mu +=
5840  +121947. * CiHbox / LambdaNP2
5841  +713174. * CiHL1_11 / LambdaNP2
5842  -53393.3 * CiHe_11 / LambdaNP2
5843  +713174. * CiHL3_11 / LambdaNP2
5844  -111120. * CiHD / LambdaNP2
5845  +843388. * CiHB / LambdaNP2
5846  +417838. * CiHW / LambdaNP2
5847  -386753. * CiHWB / LambdaNP2
5848  -27915.7 * CiDHB / LambdaNP2
5849  +11946.5 * CiDHW / LambdaNP2
5850  -5.496 * DeltaGF()
5851  ;
5852 
5853  // Add modifications due to small variations of the SM parameters
5854  mu += cHSM * ( +6.641 * deltaMz()
5855  -4.576 * deltaMh()
5856  -2.605 * deltaaMZ()
5857  +5.56 * deltaGmu() );
5858 
5859  } else {
5860  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
5861  }
5862 
5863  } else if (sqrt_s == 0.350) {
5864 
5865  C1 = 0.0069;
5866 
5867  if (Pol_em == 80. && Pol_ep == -30.){
5868  mu +=
5869  +121674. * CiHbox / LambdaNP2
5870  -47420.2 * CiHL1_11 / LambdaNP2
5871  -172088. * CiHe_11 / LambdaNP2
5872  -47420.2 * CiHL3_11 / LambdaNP2
5873  +59728. * CiHD / LambdaNP2
5874  +544205. * CiHB / LambdaNP2
5875  +83604.4 * CiHW / LambdaNP2
5876  +435393. * CiHWB / LambdaNP2
5877  -24800.4 * CiDHB / LambdaNP2
5878  -4583.09 * CiDHW / LambdaNP2
5879  -0.05 * DeltaGF()
5880  ;
5881 
5882  // Add modifications due to small variations of the SM parameters
5883  mu += cHSM * ( -2.905 * deltaMz()
5884  -1.842 * deltaMh()
5885  +2.966 * deltaaMZ()
5886  +0.009 * deltaGmu() );
5887 
5888  } else if (Pol_em == -80. && Pol_ep == 30.){
5889  mu +=
5890  +121541. * CiHbox / LambdaNP2
5891  +197618. * CiHL1_11 / LambdaNP2
5892  +42238.9 * CiHe_11 / LambdaNP2
5893  +197618. * CiHL3_11 / LambdaNP2
5894  -124376. * CiHD / LambdaNP2
5895  +181154. * CiHB / LambdaNP2
5896  +195329. * CiHW / LambdaNP2
5897  -505800. * CiHWB / LambdaNP2
5898  +13082.6 * CiDHB / LambdaNP2
5899  -26607.4 * CiDHW / LambdaNP2
5900  -6.096 * DeltaGF()
5901  ;
5902 
5903  // Add modifications due to small variations of the SM parameters
5904  mu += cHSM * ( +9.303 * deltaMz()
5905  -1.82 * deltaMh()
5906  -3.105 * deltaaMZ()
5907  +6.071 * deltaGmu() );
5908 
5909  } else if (Pol_em == 80. && Pol_ep == 0.){
5910  mu +=
5911  +121760. * CiHbox / LambdaNP2
5912  -62853. * CiHL1_11 / LambdaNP2
5913  -83019.6 * CiHe_11 / LambdaNP2
5914  -62853. * CiHL3_11 / LambdaNP2
5915  +34395.4 * CiHD / LambdaNP2
5916  +623389. * CiHB / LambdaNP2
5917  +123932. * CiHW / LambdaNP2
5918  +181789. * CiHWB / LambdaNP2
5919  -20420. * CiDHB / LambdaNP2
5920  -7820.42 * CiDHW / LambdaNP2
5921  -0.875 * DeltaGF()
5922  ;
5923 
5924  // Add modifications due to small variations of the SM parameters
5925  mu += cHSM * ( -1.322 * deltaMz()
5926  -1.873 * deltaMh()
5927  +2.14 * deltaaMZ()
5928  +0.844 * deltaGmu() );
5929 
5930  } else if (Pol_em == -80. && Pol_ep == 0.){
5931  mu +=
5932  +121557. * CiHbox / LambdaNP2
5933  +131443. * CiHL1_11 / LambdaNP2
5934  +63326.7 * CiHe_11 / LambdaNP2
5935  +131443. * CiHL3_11 / LambdaNP2
5936  -103038. * CiHD / LambdaNP2
5937  +323596. * CiHB / LambdaNP2
5938  +201676. * CiHW / LambdaNP2
5939  -491019. * CiHWB / LambdaNP2
5940  +7992.43 * CiDHB / LambdaNP2
5941  -24283.6 * CiDHW / LambdaNP2
5942  -5.391 * DeltaGF()
5943  ;
5944 
5945  // Add modifications due to small variations of the SM parameters
5946  mu += cHSM * ( +7.818 * deltaMz()
5947  -1.846 * deltaMh()
5948  -2.402 * deltaaMZ()
5949  +5.358 * deltaGmu() );
5950 
5951  } else {
5952  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
5953  }
5954 
5955  } else if (sqrt_s == 0.365) {
5956 
5957  C1 = 0.0069; // Use same as 350 GeV
5958 
5959  if (Pol_em == 80. && Pol_ep == -30.){
5960  mu +=
5961  +121458. * CiHbox / LambdaNP2
5962  -58695.1 * CiHL1_11 / LambdaNP2
5963  -109686. * CiHe_11 / LambdaNP2
5964  -58695.1 * CiHL3_11 / LambdaNP2
5965  +58496.7 * CiHD / LambdaNP2
5966  +489137. * CiHB / LambdaNP2
5967  +80751.3 * CiHW / LambdaNP2
5968  +410304. * CiHWB / LambdaNP2
5969  -30918.3 * CiDHB / LambdaNP2
5970  -3571.31 * CiDHW / LambdaNP2
5971  -0.085 * DeltaGF()
5972  ;
5973 
5974  // Add modifications due to small variations of the SM parameters
5975  mu += cHSM * ( -2.809 * deltaMz()
5976  -1.721 * deltaMh()
5977  +2.93 * deltaaMZ()
5978  +0.026 * deltaGmu() );
5979 
5980  } else if (Pol_em == -80. && Pol_ep == 30.){
5981  mu +=
5982  +121152. * CiHbox / LambdaNP2
5983  +136019. * CiHL1_11 / LambdaNP2
5984  +50762. * CiHe_11 / LambdaNP2
5985  +136019. * CiHL3_11 / LambdaNP2
5986  -123859. * CiHD / LambdaNP2
5987  +165799. * CiHB / LambdaNP2
5988  +176652. * CiHW / LambdaNP2
5989  -504889. * CiHWB / LambdaNP2
5990  +16920.7 * CiDHB / LambdaNP2
5991  -31414.1 * CiDHW / LambdaNP2
5992  -6.076 * DeltaGF()
5993  ;
5994 
5995  // Add modifications due to small variations of the SM parameters
5996  mu += cHSM * ( +9.271 * deltaMz()
5997  -1.7 * deltaMh()
5998  -3.092 * deltaaMZ()
5999  +6.031 * deltaGmu() );
6000 
6001  } else if (Pol_em == 80. && Pol_ep == 0.){
6002  mu +=
6003  +121193. * CiHbox / LambdaNP2
6004  -76905.7 * CiHL1_11 / LambdaNP2
6005  -32264.3 * CiHe_11 / LambdaNP2
6006  -76905.7 * CiHL3_11 / LambdaNP2
6007  +33650.3 * CiHD / LambdaNP2
6008  +573505. * CiHB / LambdaNP2
6009  +117937. * CiHW / LambdaNP2
6010  +166382. * CiHWB / LambdaNP2
6011  -25012.1 * CiDHB / LambdaNP2
6012  -7703.47 * CiDHW / LambdaNP2
6013  -0.911 * DeltaGF()
6014  ;
6015 
6016  // Add modifications due to small variations of the SM parameters
6017  mu += cHSM * ( -1.233 * deltaMz()
6018  -1.746 * deltaMh()
6019  +2.101 * deltaaMZ()
6020  +0.861 * deltaGmu() );
6021 
6022  } else if (Pol_em == -80. && Pol_ep == 0.){
6023  mu +=
6024  +121177. * CiHbox / LambdaNP2
6025  +77981.5 * CiHL1_11 / LambdaNP2
6026  +74274.1 * CiHe_11 / LambdaNP2
6027  +77981.5 * CiHL3_11 / LambdaNP2
6028  -102068. * CiHD / LambdaNP2
6029  +305730. * CiHB / LambdaNP2
6030  +183682. * CiHW / LambdaNP2
6031  -487770. * CiHWB / LambdaNP2
6032  +10624.8 * CiDHB / LambdaNP2
6033  -28092.3 * CiDHW / LambdaNP2
6034  -5.366 * DeltaGF()
6035  ;
6036 
6037  // Add modifications due to small variations of the SM parameters
6038  mu += cHSM * ( +7.791 * deltaMz()
6039  -1.726 * deltaMh()
6040  -2.377 * deltaaMZ()
6041  +5.325 * deltaGmu() );
6042 
6043  } else {
6044  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
6045  }
6046 
6047  } else if (sqrt_s == 0.380) {
6048 
6049  C1 = 0.0069; // Use same as 350 GeV
6050 
6051  if (Pol_em == 80. && Pol_ep == -30.){
6052  mu +=
6053  +121392. * CiHbox / LambdaNP2
6054  -68799.8 * CiHL1_11 / LambdaNP2
6055  -54383.2 * CiHe_11 / LambdaNP2
6056  -68799.8 * CiHL3_11 / LambdaNP2
6057  +57427.7 * CiHD / LambdaNP2
6058  +439155. * CiHB / LambdaNP2
6059  +76978.2 * CiHW / LambdaNP2
6060  +392293. * CiHWB / LambdaNP2
6061  -36175.9 * CiDHB / LambdaNP2
6062  -3193.74 * CiDHW / LambdaNP2
6063  -0.11 * DeltaGF()
6064  ;
6065 
6066  // Add modifications due to small variations of the SM parameters
6067  mu += cHSM * ( -2.74 * deltaMz()
6068  -1.62 * deltaMh()
6069  +2.907 * deltaaMZ()
6070  +0.079 * deltaGmu() );
6071 
6072  } else if (Pol_em == -80. && Pol_ep == 30.){
6073  mu +=
6074  +121306. * CiHbox / LambdaNP2
6075  +80159.7 * CiHL1_11 / LambdaNP2
6076  +58002.2 * CiHe_11 / LambdaNP2
6077  +80159.7 * CiHL3_11 / LambdaNP2
6078  -123524. * CiHD / LambdaNP2
6079  +151617. * CiHB / LambdaNP2
6080  +154342. * CiHW / LambdaNP2
6081  -500961. * CiHWB / LambdaNP2
6082  +20509.9 * CiDHB / LambdaNP2
6083  -35718.1 * CiDHW / LambdaNP2
6084  -6.064 * DeltaGF()
6085  ;
6086 
6087  // Add modifications due to small variations of the SM parameters
6088  mu += cHSM * ( +9.254 * deltaMz()
6089  -1.608 * deltaMh()
6090  -3.07 * deltaaMZ()
6091  +6.04 * deltaGmu() );
6092 
6093  } else if (Pol_em == 80. && Pol_ep == 0.){
6094  mu +=
6095  +121171. * CiHbox / LambdaNP2
6096  -89494.3 * CiHL1_11 / LambdaNP2
6097  +11882.3 * CiHe_11 / LambdaNP2
6098  -89494.3 * CiHL3_11 / LambdaNP2
6099  +32430.1 * CiHD / LambdaNP2
6100  +524620. * CiHB / LambdaNP2
6101  +111520. * CiHW / LambdaNP2
6102  +156122. * CiHWB / LambdaNP2
6103  -29271.1 * CiDHB / LambdaNP2
6104  -8056.8 * CiDHW / LambdaNP2
6105  -0.928 * DeltaGF()
6106  ;
6107 
6108  // Add modifications due to small variations of the SM parameters
6109  mu += cHSM * ( -1.145 * deltaMz()
6110  -1.643 * deltaMh()
6111  +2.077 * deltaaMZ()
6112  +0.898 * deltaGmu() );
6113 
6114  } else if (Pol_em == -80. && Pol_ep == 0.){
6115  mu +=
6116  +121286. * CiHbox / LambdaNP2
6117  +30046.7 * CiHL1_11 / LambdaNP2
6118  +84014. * CiHe_11 / LambdaNP2
6119  +30046.7 * CiHL3_11 / LambdaNP2
6120  -101539. * CiHD / LambdaNP2
6121  +286981. * CiHB / LambdaNP2
6122  +164662. * CiHW / LambdaNP2
6123  -480410. * CiHWB / LambdaNP2
6124  +13149.6 * CiDHB / LambdaNP2
6125  -31886.7 * CiDHW / LambdaNP2
6126  -5.346 * DeltaGF()
6127  ;
6128 
6129  // Add modifications due to small variations of the SM parameters
6130  mu += cHSM * ( +7.766 * deltaMz()
6131  -1.629 * deltaMh()
6132  -2.353 * deltaaMZ()
6133  +5.316 * deltaGmu() );
6134 
6135  } else {
6136  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
6137  }
6138 
6139  } else if (sqrt_s == 0.500) {
6140 
6141  C1 = 0.0067;
6142 
6143  if (Pol_em == 80. && Pol_ep == -30.){
6144  mu +=
6145  +121372. * CiHbox / LambdaNP2
6146  -121062. * CiHL1_11 / LambdaNP2
6147  +224754. * CiHe_11 / LambdaNP2
6148  -121062. * CiHL3_11 / LambdaNP2
6149  +55161.7 * CiHD / LambdaNP2
6150  +201238. * CiHB / LambdaNP2
6151  +52456.6 * CiHW / LambdaNP2
6152  +335517. * CiHWB / LambdaNP2
6153  -63733.4 * CiDHB / LambdaNP2
6154  -2379.21 * CiDHW / LambdaNP2
6155  -0.207 * DeltaGF()
6156  ;
6157 
6158  // Add modifications due to small variations of the SM parameters
6159  mu += cHSM * ( -2.453 * deltaMz()
6160  -1.136 * deltaMh()
6161  +2.81 * deltaaMZ()
6162  +0.175 * deltaGmu() );
6163 
6164  } else if (Pol_em == -80. && Pol_ep == 30.){
6165  mu +=
6166  +121399. * CiHbox / LambdaNP2
6167  -200849. * CiHL1_11 / LambdaNP2
6168  +96427.7 * CiHe_11 / LambdaNP2
6169  -200849. * CiHL3_11 / LambdaNP2
6170  -121178. * CiHD / LambdaNP2
6171  +83220.9 * CiHB / LambdaNP2
6172  +42832.2 * CiHW / LambdaNP2
6173  -464173. * CiHWB / LambdaNP2
6174  +37654.2 * CiDHB / LambdaNP2
6175  -59029.6 * CiDHW / LambdaNP2
6176  -6.025 * DeltaGF()
6177  ;
6178 
6179  // Add modifications due to small variations of the SM parameters
6180  mu += cHSM * ( +9.205 * deltaMz()
6181  -1.133 * deltaMh()
6182  -3.019 * deltaaMZ()
6183  +5.99 * deltaGmu() );
6184 
6185  } else if (Pol_em == 80. && Pol_ep == 0.){
6186  mu +=
6187  +121435. * CiHbox / LambdaNP2
6188  -154953. * CiHL1_11 / LambdaNP2
6189  +235326. * CiHe_11 / LambdaNP2
6190  -154953. * CiHL3_11 / LambdaNP2
6191  +30472. * CiHD / LambdaNP2
6192  +298145. * CiHB / LambdaNP2
6193  +75047.6 * CiHW / LambdaNP2
6194  +137304. * CiHWB / LambdaNP2
6195  -49636.1 * CiDHB / LambdaNP2
6196  -10277.1 * CiDHW / LambdaNP2
6197  -1.027 * DeltaGF()
6198  ;
6199 
6200  // Add modifications due to small variations of the SM parameters
6201  mu += cHSM * ( -0.829 * deltaMz()
6202  -1.142 * deltaMh()
6203  +1.988 * deltaaMZ()
6204  +0.989 * deltaGmu() );
6205 
6206  } else if (Pol_em == -80. && Pol_ep == 0.){
6207  mu +=
6208  +121468. * CiHbox / LambdaNP2
6209  -208577. * CiHL1_11 / LambdaNP2
6210  +134790. * CiHe_11 / LambdaNP2
6211  -208577. * CiHL3_11 / LambdaNP2
6212  -98708.1 * CiHD / LambdaNP2
6213  +190310. * CiHB / LambdaNP2
6214  +62321.4 * CiHW / LambdaNP2
6215  -429412. * CiHWB / LambdaNP2
6216  +24628.2 * CiDHB / LambdaNP2
6217  -51722.9 * CiDHW / LambdaNP2
6218  -5.287 * DeltaGF()
6219  ;
6220 
6221  // Add modifications due to small variations of the SM parameters
6222  mu += cHSM * ( +7.714 * deltaMz()
6223  -1.14 * deltaMh()
6224  -2.279 * deltaaMZ()
6225  +5.251 * deltaGmu() );
6226 
6227  } else {
6228  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
6229  }
6230 
6231  } else if (sqrt_s == 1.0) {
6232 
6233  C1 = 0.0065;
6234 
6235  if (Pol_em == 80. && Pol_ep == -30.){
6236  mu +=
6237  +121044. * CiHbox / LambdaNP2
6238  -206156. * CiHL1_11 / LambdaNP2
6239  +586357. * CiHe_11 / LambdaNP2
6240  -206156. * CiHL3_11 / LambdaNP2
6241  +54157.3 * CiHD / LambdaNP2
6242  -30839.6 * CiHB / LambdaNP2
6243  +18110.3 * CiHW / LambdaNP2
6244  +345253. * CiHWB / LambdaNP2
6245  -108488. * CiDHB / LambdaNP2
6246  -12324.2 * CiDHW / LambdaNP2
6247  -0.229 * DeltaGF()
6248  ;
6249 
6250  // Add modifications due to small variations of the SM parameters
6251  mu += cHSM * ( -2.141 * deltaMz()
6252  -0.544 * deltaMh()
6253  +2.775 * deltaaMZ()
6254  +0.211 * deltaGmu() );
6255 
6256  } else if (Pol_em == -80. && Pol_ep == 30.){
6257  mu +=
6258  +121085. * CiHbox / LambdaNP2
6259  -565700. * CiHL1_11 / LambdaNP2
6260  +157498. * CiHe_11 / LambdaNP2
6261  -565700. * CiHL3_11 / LambdaNP2
6262  -120795. * CiHD / LambdaNP2
6263  +7953.6 * CiHB / LambdaNP2
6264  -79908.9 * CiHW / LambdaNP2
6265  -402278. * CiHWB / LambdaNP2
6266  +54805.3 * CiDHB / LambdaNP2
6267  -101988. * CiDHW / LambdaNP2
6268  -6.001 * DeltaGF()
6269  ;
6270 
6271  // Add modifications due to small variations of the SM parameters
6272  mu += cHSM * ( +9.412 * deltaMz()
6273  -0.546 * deltaMh()
6274  -3.005 * deltaaMZ()
6275  +5.986 * deltaGmu() );
6276 
6277  } else if (Pol_em == 80. && Pol_ep == -20.){
6278  mu +=
6279  +121091. * CiHbox / LambdaNP2
6280  -225779. * CiHL1_11 / LambdaNP2
6281  +568149. * CiHe_11 / LambdaNP2
6282  -225779. * CiHL3_11 / LambdaNP2
6283  +45736.7 * CiHD / LambdaNP2
6284  +2164.38 * CiHB / LambdaNP2
6285  +20504.6 * CiHW / LambdaNP2
6286  +290141. * CiHWB / LambdaNP2
6287  -100416. * CiDHB / LambdaNP2
6288  -16574.6 * CiDHW / LambdaNP2
6289  -0.51 * DeltaGF()
6290  ;
6291 
6292  // Add modifications due to small variations of the SM parameters
6293  mu += cHSM * ( -1.569 * deltaMz()
6294  -0.555 * deltaMh()
6295  +2.507 * deltaaMZ()
6296  +0.493 * deltaGmu() );
6297 
6298  } else if (Pol_em == -80. && Pol_ep == 20.){
6299  mu +=
6300  +121091. * CiHbox / LambdaNP2
6301  -552286. * CiHL1_11 / LambdaNP2
6302  +177286. * CiHe_11 / LambdaNP2
6303  -552286. * CiHL3_11 / LambdaNP2
6304  -113484. * CiHD / LambdaNP2
6305  +29757.9 * CiHB / LambdaNP2
6306  -69897.4 * CiHW / LambdaNP2
6307  -385087. * CiHWB / LambdaNP2
6308  +47999.3 * CiDHB / LambdaNP2
6309  -98310.4 * CiDHW / LambdaNP2
6310  -5.76 * DeltaGF()
6311  ;
6312 
6313  // Add modifications due to small variations of the SM parameters
6314  mu += cHSM * ( +8.942 * deltaMz()
6315  -0.556 * deltaMh()
6316  -2.75 * deltaaMZ()
6317  +5.748 * deltaGmu() );
6318 
6319  } else if (Pol_em == 80. && Pol_ep == 0.){
6320  mu +=
6321  +120996. * CiHbox / LambdaNP2
6322  -263143. * CiHL1_11 / LambdaNP2
6323  +533190. * CiHe_11 / LambdaNP2
6324  -263143. * CiHL3_11 / LambdaNP2
6325  +29434.5 * CiHD / LambdaNP2
6326  +63176.5 * CiHB / LambdaNP2
6327  +26728.5 * CiHW / LambdaNP2
6328  +184228. * CiHWB / LambdaNP2
6329  -85487.1 * CiDHB / LambdaNP2
6330  -24906.1 * CiDHW / LambdaNP2
6331  -1.044 * DeltaGF()
6332  ;
6333 
6334  // Add modifications due to small variations of the SM parameters
6335  mu += cHSM * ( -0.508 * deltaMz()
6336  -0.545 * deltaMh()
6337  +1.958 * deltaaMZ()
6338  +1.027 * deltaGmu() );
6339 
6340  } else if (Pol_em == -80. && Pol_ep == 0.){
6341  mu +=
6342  +121114. * CiHbox / LambdaNP2
6343  -524119. * CiHL1_11 / LambdaNP2
6344  +218758. * CiHe_11 / LambdaNP2
6345  -524119. * CiHL3_11 / LambdaNP2
6346  -98164. * CiHD / LambdaNP2
6347  +74694.7 * CiHB / LambdaNP2
6348  -49060.4 * CiHW / LambdaNP2
6349  -348619. * CiHWB / LambdaNP2
6350  +33861.6 * CiDHB / LambdaNP2
6351  -90369.8 * CiDHW / LambdaNP2
6352  -5.256 * DeltaGF()
6353  ;
6354 
6355  // Add modifications due to small variations of the SM parameters
6356  mu += cHSM * ( +7.922 * deltaMz()
6357  -0.546 * deltaMh()
6358  -2.261 * deltaaMZ()
6359  +5.242 * deltaGmu() );
6360 
6361  } else {
6362  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
6363  }
6364 
6365  } else if (sqrt_s == 1.4) {
6366 
6367  C1 = 0.0065;
6368 
6369  if (Pol_em == 80. && Pol_ep == -30.){
6370  mu +=
6371  +120762. * CiHbox / LambdaNP2
6372  -242720. * CiHL1_11 / LambdaNP2
6373  +714345. * CiHe_11 / LambdaNP2
6374  -242720. * CiHL3_11 / LambdaNP2
6375  +53823.3 * CiHD / LambdaNP2
6376  -64876.7 * CiHB / LambdaNP2
6377  +9362.37 * CiHW / LambdaNP2
6378  +355440. * CiHWB / LambdaNP2
6379  -127361. * CiDHB / LambdaNP2
6380  -18147.3 * CiDHW / LambdaNP2
6381  -0.228 * DeltaGF()
6382  ;
6383 
6384  // Add modifications due to small variations of the SM parameters
6385  mu += cHSM * ( -2.05 * deltaMz()
6386  -0.422 * deltaMh()
6387  +2.78 * deltaaMZ()
6388  +0.2 * deltaGmu() );
6389 
6390  } else if (Pol_em == -80. && Pol_ep == 30.){
6391  mu +=
6392  +120818. * CiHbox / LambdaNP2
6393  -692905. * CiHL1_11 / LambdaNP2
6394  +184416. * CiHe_11 / LambdaNP2
6395  -692905. * CiHL3_11 / LambdaNP2
6396  -121143. * CiHD / LambdaNP2
6397  -4989.81 * CiHB / LambdaNP2
6398  -93241.6 * CiHW / LambdaNP2
6399  -392394. * CiHWB / LambdaNP2
6400  +60556.9 * CiDHB / LambdaNP2
6401  -121409. * CiDHW / LambdaNP2
6402  -6.003 * DeltaGF()
6403  ;
6404 
6405  // Add modifications due to small variations of the SM parameters
6406  mu += cHSM * ( +9.501 * deltaMz()
6407  -0.422 * deltaMh()
6408  -2.999 * deltaaMZ()
6409  +5.972 * deltaGmu() );
6410 
6411  } else if (Pol_em == 80. && Pol_ep == 0.){
6412  mu +=
6413  +120773. * CiHbox / LambdaNP2
6414  -309806. * CiHL1_11 / LambdaNP2
6415  +643900. * CiHe_11 / LambdaNP2
6416  -309806. * CiHL3_11 / LambdaNP2
6417  +29091.1 * CiHD / LambdaNP2
6418  +22438.3 * CiHB / LambdaNP2
6419  +16021.7 * CiHW / LambdaNP2
6420  +202496. * CiHWB / LambdaNP2
6421  -100775. * CiDHB / LambdaNP2
6422  -32830.8 * CiDHW / LambdaNP2
6423  -1.043 * DeltaGF()
6424  ;
6425 
6426  // Add modifications due to small variations of the SM parameters
6427  mu += cHSM * ( -0.415 * deltaMz()
6428  -0.422 * deltaMh()
6429  +1.961 * deltaaMZ()
6430  +1.014 * deltaGmu() );
6431 
6432  } else if (Pol_em == -80. && Pol_ep == 0.){
6433  mu +=
6434  +120795. * CiHbox / LambdaNP2
6435  -637584. * CiHL1_11 / LambdaNP2
6436  +256188. * CiHe_11 / LambdaNP2
6437  -637584. * CiHL3_11 / LambdaNP2
6438  -98543.3 * CiHD / LambdaNP2
6439  +49040.2 * CiHB / LambdaNP2
6440  -63051.7 * CiHW / LambdaNP2
6441  -332850. * CiHWB / LambdaNP2
6442  +36510.1 * CiDHB / LambdaNP2
6443  -108018. * CiDHW / LambdaNP2
6444  -5.256 * DeltaGF()
6445  ;
6446 
6447  // Add modifications due to small variations of the SM parameters
6448  mu += cHSM * ( +8.01 * deltaMz()
6449  -0.423 * deltaMh()
6450  -2.255 * deltaaMZ()
6451  +5.227 * deltaGmu() );
6452 
6453  } else {
6454  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
6455  }
6456 
6457  } else if (sqrt_s == 1.5) {
6458 
6459  C1 = 0.0065;// Use the same as 1400 GeV
6460 
6461  if (Pol_em == 80. && Pol_ep == -30.){
6462  mu +=
6463  +120570. * CiHbox / LambdaNP2
6464  -250340. * CiHL1_11 / LambdaNP2
6465  +739684. * CiHe_11 / LambdaNP2
6466  -250340. * CiHL3_11 / LambdaNP2
6467  +53685.8 * CiHD / LambdaNP2
6468  -71192.9 * CiHB / LambdaNP2
6469  +9743.41 * CiHW / LambdaNP2
6470  +357556. * CiHWB / LambdaNP2
6471  -131206. * CiDHB / LambdaNP2
6472  -19448. * CiDHW / LambdaNP2
6473  -0.224 * DeltaGF()
6474  ;
6475 
6476  // Add modifications due to small variations of the SM parameters
6477  mu += cHSM * ( -2.032 * deltaMz()
6478  -0.4 * deltaMh()
6479  +2.778 * deltaaMZ()
6480  +0.194 * deltaGmu() );
6481 
6482  } else if (Pol_em == -80. && Pol_ep == 30.){
6483  mu +=
6484  +120602. * CiHbox / LambdaNP2
6485  -718001. * CiHL1_11 / LambdaNP2
6486  +189852. * CiHe_11 / LambdaNP2
6487  -718001. * CiHL3_11 / LambdaNP2
6488  -121214. * CiHD / LambdaNP2
6489  -6057.91 * CiHB / LambdaNP2
6490  -95148.1 * CiHW / LambdaNP2
6491  -390958. * CiHWB / LambdaNP2
6492  +61690.7 * CiDHB / LambdaNP2
6493  -125382. * CiDHW / LambdaNP2
6494  -5.997 * DeltaGF()
6495  ;
6496 
6497  // Add modifications due to small variations of the SM parameters
6498  mu += cHSM * ( +9.519 * deltaMz()
6499  -0.399 * deltaMh()
6500  -3.001 * deltaaMZ()
6501  +5.965 * deltaGmu() );
6502 
6503  } else if (Pol_em == 80. && Pol_ep == 0.){
6504  mu +=
6505  +120563. * CiHbox / LambdaNP2
6506  -319378. * CiHL1_11 / LambdaNP2
6507  +665765. * CiHe_11 / LambdaNP2
6508  -319378. * CiHL3_11 / LambdaNP2
6509  +29010.7 * CiHD / LambdaNP2
6510  +14190.4 * CiHB / LambdaNP2
6511  +16080. * CiHW / LambdaNP2
6512  +205187. * CiHWB / LambdaNP2
6513  -103927. * CiDHB / LambdaNP2
6514  -34420.2 * CiDHW / LambdaNP2
6515  -1.04 * DeltaGF()
6516  ;
6517 
6518  // Add modifications due to small variations of the SM parameters
6519  mu += cHSM * ( -0.398 * deltaMz()
6520  -0.4 * deltaMh()
6521  +1.96 * deltaaMZ()
6522  +1.01 * deltaGmu() );
6523 
6524  } else if (Pol_em == -80. && Pol_ep == 0.){
6525  mu +=
6526  +120607. * CiHbox / LambdaNP2
6527  -659879. * CiHL1_11 / LambdaNP2
6528  +263841. * CiHe_11 / LambdaNP2
6529  -659879. * CiHL3_11 / LambdaNP2
6530  -98617.3 * CiHD / LambdaNP2
6531  +46418.4 * CiHB / LambdaNP2
6532  -64166.6 * CiHW / LambdaNP2
6533  -330855. * CiHWB / LambdaNP2
6534  +36774.5 * CiDHB / LambdaNP2
6535  -111573. * CiDHW / LambdaNP2
6536  -5.253 * DeltaGF()
6537  ;
6538 
6539  // Add modifications due to small variations of the SM parameters
6540  mu += cHSM * ( +8.03 * deltaMz()
6541  -0.4 * deltaMh()
6542  -2.257 * deltaaMZ()
6543  +5.221 * deltaGmu() );
6544 
6545  } else {
6546  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
6547  }
6548 
6549  } else if (sqrt_s == 3.0) {
6550 
6551  C1 = 0.0063;
6552 
6553  if (Pol_em == 80. && Pol_ep == -30.){
6554  mu +=
6555  +120539. * CiHbox / LambdaNP2
6556  -327096. * CiHL1_11 / LambdaNP2
6557  +988310. * CiHe_11 / LambdaNP2
6558  -327096. * CiHL3_11 / LambdaNP2
6559  +53758.1 * CiHD / LambdaNP2
6560  -79161. * CiHB / LambdaNP2
6561  +3856.87 * CiHW / LambdaNP2
6562  +369878. * CiHWB / LambdaNP2
6563  -170059. * CiDHB / LambdaNP2
6564  -32235.8 * CiDHW / LambdaNP2
6565  -0.226 * DeltaGF()
6566  ;
6567 
6568  // Add modifications due to small variations of the SM parameters
6569  mu += cHSM * ( -1.896 * deltaMz()
6570  -0.264 * deltaMh()
6571  +2.778 * deltaaMZ()
6572  +0.174 * deltaGmu() );
6573 
6574  } else if (Pol_em == -80. && Pol_ep == 30.){
6575  mu +=
6576  +120565. * CiHbox / LambdaNP2
6577  -961658. * CiHL1_11 / LambdaNP2
6578  +247947. * CiHe_11 / LambdaNP2
6579  -961658. * CiHL3_11 / LambdaNP2
6580  -121230. * CiHD / LambdaNP2
6581  -10752.9 * CiHB / LambdaNP2
6582  -92123.7 * CiHW / LambdaNP2
6583  -391807. * CiHWB / LambdaNP2
6584  +73242.2 * CiDHB / LambdaNP2
6585  -165690. * CiDHW / LambdaNP2
6586  -6.002 * DeltaGF()
6587  ;
6588 
6589  // Add modifications due to small variations of the SM parameters
6590  mu += cHSM * ( +9.659 * deltaMz()
6591  -0.264 * deltaMh()
6592  -3.003 * deltaaMZ()
6593  +5.943 * deltaGmu() );
6594 
6595  } else if (Pol_em == 80. && Pol_ep == 0.){
6596  mu +=
6597  +120534. * CiHbox / LambdaNP2
6598  -417962. * CiHL1_11 / LambdaNP2
6599  +884851. * CiHe_11 / LambdaNP2
6600  -417962. * CiHL3_11 / LambdaNP2
6601  +29065.5 * CiHD / LambdaNP2
6602  -10885.4 * CiHB / LambdaNP2
6603  +8249.25 * CiHW / LambdaNP2
6604  +228820. * CiHWB / LambdaNP2
6605  -135851. * CiDHB / LambdaNP2
6606  -51177.2 * CiDHW / LambdaNP2
6607  -1.04 * DeltaGF()
6608  ;
6609 
6610  // Add modifications due to small variations of the SM parameters
6611  mu += cHSM * ( -0.262 * deltaMz()
6612  -0.264 * deltaMh()
6613  +1.959 * deltaaMZ()
6614  +0.987 * deltaGmu() );
6615 
6616  } else if (Pol_em == -80. && Pol_ep == 0.){
6617  mu +=
6618  +120480. * CiHbox / LambdaNP2
6619  -880604. * CiHL1_11 / LambdaNP2
6620  +344657. * CiHe_11 / LambdaNP2
6621  -880604. * CiHL3_11 / LambdaNP2
6622  -98656.8 * CiHD / LambdaNP2
6623  +28681.4 * CiHB / LambdaNP2
6624  -66216.6 * CiHW / LambdaNP2
6625  -320715. * CiHWB / LambdaNP2
6626  +41721.6 * CiDHB / LambdaNP2
6627  -148698. * CiDHW / LambdaNP2
6628  -5.256 * DeltaGF()
6629  ;
6630 
6631  // Add modifications due to small variations of the SM parameters
6632  mu += cHSM * ( +8.169 * deltaMz()
6633  -0.264 * deltaMh()
6634  -2.259 * deltaaMZ()
6635  +5.202 * deltaGmu() );
6636 
6637  } else {
6638  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
6639  }
6640 
6641  } else
6642  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
6643 
6644  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
6645  //(Assume similar to WBF.)
6646  mu += eeeWBFint + eeeWBFpar;
6647 
6648 // Linear contribution from Higgs self-coupling
6649  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
6650 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
6652 
6653  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
6654 
6655  return mu;
6656 }

◆ mueeZH()

double NPSMEFTd6::mueeZH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{eeZH}\) between the \(e^{+}e^{-}\to ZH\) associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{eeZH}\)

Reimplemented from NPbase.

Definition at line 7229 of file NPSMEFTd6.cpp.

7230 {
7231  double mu = 1.0;
7232 
7233  double C1 = 0.0;
7234 
7235  if (sqrt_s == 0.240) {
7236 
7237  C1 = 0.017;
7238 
7239  mu +=
7240  +121263. * CiHbox / LambdaNP2
7241  +898682. * CiHL1_11 / LambdaNP2
7242  -767820. * CiHe_11 / LambdaNP2
7243  +898682. * CiHL3_11 / LambdaNP2
7244  -6046.36 * CiHD / LambdaNP2
7245  +122439. * CiHB / LambdaNP2
7246  +540057. * CiHW / LambdaNP2
7247  +231063. * CiHWB / LambdaNP2
7248  +17593.2 * CiDHB / LambdaNP2
7249  +53409.5 * CiDHW / LambdaNP2
7250  -2.2 * DeltaGF()
7251  ;
7252 
7253  // Add modifications due to small variations of the SM parameters
7254  mu += cHSM * ( -0.2 * deltaaMZ()
7255  +2.2 * deltaGmu()
7256  +4.775 * deltaMz()
7257  -3.071 * deltaMh() );
7258 
7259  if (FlagQuadraticTerms) {
7260  //Add contributions that are quadratic in the effective coefficients
7261  mu += 0.0;
7262  }
7263 
7264  } else if (sqrt_s == 0.250) {
7265 
7266  C1 = 0.015;
7267 
7268  mu +=
7269  +121263. * CiHbox / LambdaNP2
7270  +975101. * CiHL1_11 / LambdaNP2
7271  -833750. * CiHe_11 / LambdaNP2
7272  +975101. * CiHL3_11 / LambdaNP2
7273  -6046.36 * CiHD / LambdaNP2
7274  +128443. * CiHB / LambdaNP2
7275  +568273. * CiHW / LambdaNP2
7276  +244206. * CiHWB / LambdaNP2
7277  +19818.6 * CiDHB / LambdaNP2
7278  +60127.6 * CiDHW / LambdaNP2
7279  -2.2 * DeltaGF()
7280  ;
7281 
7282  // Add modifications due to small variations of the SM parameters
7283  mu += cHSM * ( -0.2 * deltaaMZ()
7284  +2.2 * deltaGmu()
7285  +5.219 * deltaMz()
7286  -2.27 * deltaMh() );
7287 
7288  if (FlagQuadraticTerms) {
7289  //Add contributions that are quadratic in the effective coefficients
7290  mu += 0.0;
7291  }
7292 
7293  } else if (sqrt_s == 0.350) {
7294 
7295  C1 = 0.0057;
7296 
7297  mu +=
7298  +121283. * CiHbox / LambdaNP2
7299  +1911340. * CiHL1_11 / LambdaNP2
7300  -1640958. * CiHe_11 / LambdaNP2
7301  +1911340. * CiHL3_11 / LambdaNP2
7302  -6009.52 * CiHD / LambdaNP2
7303  +173183. * CiHB / LambdaNP2
7304  +785843. * CiHW / LambdaNP2
7305  +344494. * CiHWB / LambdaNP2
7306  +59158.7 * CiDHB / LambdaNP2
7307  +167954. * CiDHW / LambdaNP2
7308  -2.201 * DeltaGF()
7309  ;
7310 
7311  // Add modifications due to small variations of the SM parameters
7312  mu += cHSM * ( -0.2 * deltaaMZ()
7313  +2.2 * deltaGmu()
7314  +5.396 * deltaMz()
7315  -0.729 * deltaMh() );
7316 
7317  if (FlagQuadraticTerms) {
7318  //Add contributions that are quadratic in the effective coefficients
7319  mu += 0.0;
7320  }
7321 
7322  } else if (sqrt_s == 0.365) {
7323 
7324  C1 = 0.0057; // Use same as 350 GeV
7325 
7326  mu +=
7327  +121243. * CiHbox / LambdaNP2
7328  +2078482. * CiHL1_11 / LambdaNP2
7329  -1785085. * CiHe_11 / LambdaNP2
7330  +2078482. * CiHL3_11 / LambdaNP2
7331  -6010.65 * CiHD / LambdaNP2
7332  +178173. * CiHB / LambdaNP2
7333  +809806. * CiHW / LambdaNP2
7334  +355487. * CiHWB / LambdaNP2
7335  +67662.7 * CiDHB / LambdaNP2
7336  +190194. * CiDHW / LambdaNP2
7337  -2.201 * DeltaGF()
7338  ;
7339 
7340  // Add modifications due to small variations of the SM parameters
7341  mu += cHSM * ( -0.2 * deltaaMZ()
7342  +2.2 * deltaGmu()
7343  +5.348 * deltaMz()
7344  -0.664 * deltaMh() );
7345 
7346  if (FlagQuadraticTerms) {
7347  //Add contributions that are quadratic in the effective coefficients
7348  mu += 0.0;
7349  }
7350 
7351  } else if (sqrt_s == 0.380) {
7352 
7353  C1 = 0.0057; // Use same as 350 GeV
7354 
7355  mu +=
7356  +121281. * CiHbox / LambdaNP2
7357  +2253013. * CiHL1_11 / LambdaNP2
7358  -1934557. * CiHe_11 / LambdaNP2
7359  +2253013. * CiHL3_11 / LambdaNP2
7360  -6026.37 * CiHD / LambdaNP2
7361  +182674. * CiHB / LambdaNP2
7362  +832109. * CiHW / LambdaNP2
7363  +365819. * CiHWB / LambdaNP2
7364  +76742. * CiDHB / LambdaNP2
7365  +214030. * CiDHW / LambdaNP2
7366  -2.202 * DeltaGF()
7367  ;
7368 
7369  // Add modifications due to small variations of the SM parameters
7370  mu += cHSM * ( -0.2 * deltaaMZ()
7371  +2.2 * deltaGmu()
7372  +5.301 * deltaMz()
7373  -0.609 * deltaMh() );
7374 
7375  if (FlagQuadraticTerms) {
7376  //Add contributions that are quadratic in the effective coefficients
7377  mu += 0.0;
7378  }
7379 
7380  } else if (sqrt_s == 0.500) {
7381 
7382  C1 = 0.00099;
7383 
7384  mu +=
7385  +121264. * CiHbox / LambdaNP2
7386  +3900384. * CiHL1_11 / LambdaNP2
7387  -3350136. * CiHe_11 / LambdaNP2
7388  +3900384. * CiHL3_11 / LambdaNP2
7389  -6019.22 * CiHD / LambdaNP2
7390  +209229. * CiHB / LambdaNP2
7391  +959942. * CiHW / LambdaNP2
7392  +425112. * CiHWB / LambdaNP2
7393  +169841. * CiDHB / LambdaNP2
7394  +455437. * CiDHW / LambdaNP2
7395  -2.202 * DeltaGF()
7396  ;
7397 
7398  // Add modifications due to small variations of the SM parameters
7399  mu += cHSM * ( -0.2 * deltaaMZ()
7400  +2.2 * deltaGmu()
7401  +5. * deltaMz()
7402  -0.351 * deltaMh() );
7403 
7404  if (FlagQuadraticTerms) {
7405  //Add contributions that are quadratic in the effective coefficients
7406  mu += 0.0;
7407  }
7408 
7409  } else if (sqrt_s == 1.0) {
7410 
7411  C1 = -0.0012;
7412 
7413  mu +=
7414  +121274. * CiHbox / LambdaNP2
7415  +15601820. * CiHL1_11 / LambdaNP2
7416  -13395670. * CiHe_11 / LambdaNP2
7417  +15601820. * CiHL3_11 / LambdaNP2
7418  -6040.16 * CiHD / LambdaNP2
7419  +243960. * CiHB / LambdaNP2
7420  +1128805. * CiHW / LambdaNP2
7421  +503138. * CiHWB / LambdaNP2
7422  +899357. * CiDHB / LambdaNP2
7423  +2321619. * CiDHW / LambdaNP2
7424  -2.202 * DeltaGF()
7425  ;
7426 
7427  // Add modifications due to small variations of the SM parameters
7428  mu += cHSM * ( -0.2 * deltaaMZ()
7429  +2.2 * deltaGmu()
7430  +4.574 * deltaMz()
7431  -0.092 * deltaMh() );
7432 
7433  if (FlagQuadraticTerms) {
7434  //Add contributions that are quadratic in the effective coefficients
7435  mu += 0.0;
7436  }
7437 
7438  } else if (sqrt_s == 1.4) {
7439 
7440  C1 = -0.0011;
7441 
7442  mu +=
7443  +121283. * CiHbox / LambdaNP2
7444  +30579278. * CiHL1_11 / LambdaNP2
7445  -26253064. * CiHe_11 / LambdaNP2
7446  +30579278. * CiHL3_11 / LambdaNP2
7447  -6010.77 * CiHD / LambdaNP2
7448  +250804. * CiHB / LambdaNP2
7449  +1161208. * CiHW / LambdaNP2
7450  +518040. * CiHWB / LambdaNP2
7451  +1848758. * CiDHB / LambdaNP2
7452  +4747422. * CiDHW / LambdaNP2
7453  -2.203 * DeltaGF()
7454  ;
7455 
7456  // Add modifications due to small variations of the SM parameters
7457  mu += cHSM * ( -0.2 * deltaaMZ()
7458  +2.2 * deltaGmu()
7459  +4.491 * deltaMz()
7460  -0.047 * deltaMh() );
7461 
7462  if (FlagQuadraticTerms) {
7463  //Add contributions that are quadratic in the effective coefficients
7464  mu += 0.0;
7465  }
7466 
7467  } else if (sqrt_s == 1.5) {
7468 
7469  C1 = -0.0011;// Use the same as 1400 GeV
7470 
7471  mu +=
7472  +121262. * CiHbox / LambdaNP2
7473  +35102329. * CiHL1_11 / LambdaNP2
7474  -30135878. * CiHe_11 / LambdaNP2
7475  +35102329. * CiHL3_11 / LambdaNP2
7476  -6034.22 * CiHD / LambdaNP2
7477  +251576. * CiHB / LambdaNP2
7478  +1165634. * CiHW / LambdaNP2
7479  +519954. * CiHWB / LambdaNP2
7480  +2132554. * CiDHB / LambdaNP2
7481  +5481906. * CiDHW / LambdaNP2
7482  -2.203 * DeltaGF()
7483  ;
7484 
7485  // Add modifications due to small variations of the SM parameters
7486  mu += cHSM * ( -0.2 * deltaaMZ()
7487  +2.2 * deltaGmu()
7488  +4.479 * deltaMz()
7489  -0.041 * deltaMh() );
7490 
7491  if (FlagQuadraticTerms) {
7492  //Add contributions that are quadratic in the effective coefficients
7493  mu += 0.0;
7494  }
7495 
7496  } else if (sqrt_s == 3.0) {
7497 
7498  C1 = -0.00054;
7499 
7500  mu +=
7501  +121279. * CiHbox / LambdaNP2
7502  +140413697. * CiHL1_11 / LambdaNP2
7503  -120540988. * CiHe_11 / LambdaNP2
7504  +140413697. * CiHL3_11 / LambdaNP2
7505  -6012.61 * CiHD / LambdaNP2
7506  +257222. * CiHB / LambdaNP2
7507  +1188444. * CiHW / LambdaNP2
7508  +530503. * CiHWB / LambdaNP2
7509  +8839419. * CiDHB / LambdaNP2
7510  +22583370. * CiDHW / LambdaNP2
7511  -2.202 * DeltaGF()
7512  ;
7513 
7514  // Add modifications due to small variations of the SM parameters
7515  mu += cHSM * ( -0.2 * deltaaMZ()
7516  +2.2 * deltaGmu()
7517  +4.42 * deltaMz()
7518  -0.01 * deltaMh() );
7519 
7520  if (FlagQuadraticTerms) {
7521  //Add contributions that are quadratic in the effective coefficients
7522  mu += 0.0;
7523  }
7524 
7525  } else
7526  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZH()");
7527 
7528  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
7529  mu += eeeZHint + eeeZHpar;
7530 
7531 // Linear contribution from Higgs self-coupling
7532  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
7533 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
7535 
7536  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
7537 
7538  return mu;
7539 }

◆ mueeZHPol()

double NPSMEFTd6::mueeZHPol ( const double  sqrt_s,
const double  Pol_em,
const double  Pol_ep 
) const
virtual

The ratio \(\mu_{eeZH}\) between the \( e^{+}e^{-}\to ZH \) associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively
Returns
\(\mu_{eeZH}\)

Reimplemented from NPbase.

Definition at line 7586 of file NPSMEFTd6.cpp.

7587 {
7588  double mu = 1.0;
7589 
7590  double C1 = 0.0;
7591 
7592  if (sqrt_s == 0.240) {
7593 
7594  C1 = 0.017;
7595 
7596  if (Pol_em == 80. && Pol_ep == -30.){
7597  mu +=
7598  +121260. * CiHbox / LambdaNP2
7599  +117191. * CiHL1_11 / LambdaNP2
7600  -1681596. * CiHe_11 / LambdaNP2
7601  +117191. * CiHL3_11 / LambdaNP2
7602  +74555.1 * CiHD / LambdaNP2
7603  +528105. * CiHB / LambdaNP2
7604  +134403. * CiHW / LambdaNP2
7605  +872560. * CiHWB / LambdaNP2
7606  +137571. * CiDHB / LambdaNP2
7607  -12321.5 * CiDHW / LambdaNP2
7608  +0.459 * DeltaGF()
7609  ;
7610 
7611  // Add modifications due to small variations of the SM parameters
7612  mu += cHSM * ( +2.46 * deltaaMZ()
7613  -0.46 * deltaGmu()
7614  -0.544 * deltaMz()
7615  -3.071 * deltaMh() );
7616 
7617  } else if (Pol_em == -80. && Pol_ep == 30.){
7618  mu +=
7619  +121254. * CiHbox / LambdaNP2
7620  +1495015. * CiHL1_11 / LambdaNP2
7621  -76567.2 * CiHe_11 / LambdaNP2
7622  +1495015. * CiHL3_11 / LambdaNP2
7623  -67582.1 * CiHD / LambdaNP2
7624  -187104. * CiHB / LambdaNP2
7625  +849552. * CiHW / LambdaNP2
7626  -258537. * CiHWB / LambdaNP2
7627  -73970.1 * CiDHB / LambdaNP2
7628  +103582. * CiDHW / LambdaNP2
7629  -4.23 * DeltaGF()
7630  ;
7631 
7632  // Add modifications due to small variations of the SM parameters
7633  mu += cHSM * ( -2.23 * deltaaMZ()
7634  +4.23 * deltaGmu()
7635  +8.834 * deltaMz()
7636  -3.071 * deltaMh() );
7637 
7638  } else if (Pol_em == 80. && Pol_ep == 0.){
7639  mu +=
7640  +121256. * CiHbox / LambdaNP2
7641  +204529. * CiHL1_11 / LambdaNP2
7642  -1578998. * CiHe_11 / LambdaNP2
7643  +204529. * CiHL3_11 / LambdaNP2
7644  +65548.7 * CiHD / LambdaNP2
7645  +482729. * CiHB / LambdaNP2
7646  +179733. * CiHW / LambdaNP2
7647  +800870. * CiHWB / LambdaNP2
7648  +124170. * CiDHB / LambdaNP2
7649  -5016.48 * CiDHW / LambdaNP2
7650  +0.162 * DeltaGF()
7651  ;
7652 
7653  // Add modifications due to small variations of the SM parameters
7654  mu += cHSM * ( +2.163 * deltaaMZ()
7655  -0.163 * deltaGmu()
7656  +0.05 * deltaMz()
7657  -3.071 * deltaMh() );
7658 
7659  } else if (Pol_em == -80. && Pol_ep == 0.){
7660  mu +=
7661  +121264. * CiHbox / LambdaNP2
7662  +1442776. * CiHL1_11 / LambdaNP2
7663  -137405. * CiHe_11 / LambdaNP2
7664  +1442776. * CiHL3_11 / LambdaNP2
7665  -62167.6 * CiHD / LambdaNP2
7666  -159988. * CiHB / LambdaNP2
7667  +822448. * CiHW / LambdaNP2
7668  -215639. * CiHWB / LambdaNP2
7669  -65950.1 * CiDHB / LambdaNP2
7670  +99206.1 * CiDHW / LambdaNP2
7671  -4.052 * DeltaGF()
7672  ;
7673 
7674  // Add modifications due to small variations of the SM parameters
7675  mu += cHSM * ( -2.052 * deltaaMZ()
7676  +4.052 * deltaGmu()
7677  +8.479 * deltaMz()
7678  -3.071 * deltaMh() );
7679 
7680  } else {
7681  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
7682  }
7683 
7684  } else if (sqrt_s == 0.250) {
7685 
7686  C1 = 0.015;
7687 
7688  if (Pol_em == 80. && Pol_ep == -30.){
7689  mu +=
7690  +121264. * CiHbox / LambdaNP2
7691  +127210. * CiHL1_11 / LambdaNP2
7692  -1824910. * CiHe_11 / LambdaNP2
7693  +127210. * CiHL3_11 / LambdaNP2
7694  +74597.1 * CiHD / LambdaNP2
7695  +560319. * CiHB / LambdaNP2
7696  +136129. * CiHW / LambdaNP2
7697  +902676. * CiHWB / LambdaNP2
7698  +154358. * CiDHB / LambdaNP2
7699  -13612.9 * CiDHW / LambdaNP2
7700  +0.459 * DeltaGF()
7701  ;
7702 
7703  // Add modifications due to small variations of the SM parameters
7704  mu += cHSM * ( +2.46 * deltaaMZ()
7705  -0.46 * deltaGmu()
7706  -0.1 * deltaMz()
7707  -2.27 * deltaMh() );
7708 
7709  } else if (Pol_em == -80. && Pol_ep == 30.){
7710  mu +=
7711  +121257. * CiHbox / LambdaNP2
7712  +1622228. * CiHL1_11 / LambdaNP2
7713  -83107. * CiHe_11 / LambdaNP2
7714  +1622228. * CiHL3_11 / LambdaNP2
7715  -67554.3 * CiHD / LambdaNP2
7716  -201409. * CiHB / LambdaNP2
7717  +898116. * CiHW / LambdaNP2
7718  -258306. * CiHWB / LambdaNP2
7719  -82898. * CiDHB / LambdaNP2
7720  +116421. * CiDHW / LambdaNP2
7721  -4.23 * DeltaGF()
7722  ;
7723 
7724  // Add modifications due to small variations of the SM parameters
7725  mu += cHSM * ( -2.23 * deltaaMZ()
7726  +4.23 * deltaGmu()
7727  +9.279 * deltaMz()
7728  -2.27 * deltaMh() );
7729 
7730  } else if (Pol_em == 80. && Pol_ep == 0.){
7731  mu +=
7732  +121309. * CiHbox / LambdaNP2
7733  +221930. * CiHL1_11 / LambdaNP2
7734  -1714047. * CiHe_11 / LambdaNP2
7735  +221930. * CiHL3_11 / LambdaNP2
7736  +65599.6 * CiHD / LambdaNP2
7737  +512136. * CiHB / LambdaNP2
7738  +184424. * CiHW / LambdaNP2
7739  +829145. * CiHWB / LambdaNP2
7740  +139369. * CiDHB / LambdaNP2
7741  -5351.17 * CiDHW / LambdaNP2
7742  +0.162 * DeltaGF()
7743  ;
7744 
7745  // Add modifications due to small variations of the SM parameters
7746  mu += cHSM * ( +2.163 * deltaaMZ()
7747  -0.163 * deltaGmu()
7748  +0.494 * deltaMz()
7749  -2.27 * deltaMh() );
7750 
7751  } else if (Pol_em == -80. && Pol_ep == 0.){
7752  mu +=
7753  +121269. * CiHbox / LambdaNP2
7754  +1565559. * CiHL1_11 / LambdaNP2
7755  -148908. * CiHe_11 / LambdaNP2
7756  +1565559. * CiHL3_11 / LambdaNP2
7757  -62170. * CiHD / LambdaNP2
7758  -172540. * CiHB / LambdaNP2
7759  +869218. * CiHW / LambdaNP2
7760  -214299. * CiHWB / LambdaNP2
7761  -73929.8 * CiDHB / LambdaNP2
7762  +111494. * CiDHW / LambdaNP2
7763  -4.053 * DeltaGF()
7764  ;
7765 
7766  // Add modifications due to small variations of the SM parameters
7767  mu += cHSM * ( -2.052 * deltaaMZ()
7768  +4.052 * deltaGmu()
7769  +8.923 * deltaMz()
7770  -2.27 * deltaMh() );
7771 
7772  } else {
7773  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
7774  }
7775 
7776  } else if (sqrt_s == 0.350) {
7777 
7778  C1 = 0.0057;
7779 
7780  if (Pol_em == 80. && Pol_ep == -30.){
7781  mu +=
7782  +121274. * CiHbox / LambdaNP2
7783  +249309. * CiHL1_11 / LambdaNP2
7784  -3576996. * CiHe_11 / LambdaNP2
7785  +249309. * CiHL3_11 / LambdaNP2
7786  +74596.5 * CiHD / LambdaNP2
7787  +812491. * CiHB / LambdaNP2
7788  +146212. * CiHW / LambdaNP2
7789  +1135161. * CiHWB / LambdaNP2
7790  +395085. * CiDHB / LambdaNP2
7791  -16140.8 * CiDHW / LambdaNP2
7792  +0.458 * DeltaGF()
7793  ;
7794 
7795  // Add modifications due to small variations of the SM parameters
7796  mu += cHSM * ( +2.46 * deltaaMZ()
7797  -0.46 * deltaGmu()
7798  +0.077 * deltaMz()
7799  -0.729 * deltaMh() );
7800 
7801  } else if (Pol_em == -80. && Pol_ep == 30.){
7802  mu +=
7803  +121289. * CiHbox / LambdaNP2
7804  +3179548. * CiHL1_11 / LambdaNP2
7805  -163347. * CiHe_11 / LambdaNP2
7806  +3179548. * CiHL3_11 / LambdaNP2
7807  -67524.8 * CiHD / LambdaNP2
7808  -314653. * CiHB / LambdaNP2
7809  +1273817. * CiHW / LambdaNP2
7810  -258947. * CiHWB / LambdaNP2
7811  -197137. * CiDHB / LambdaNP2
7812  +308384. * CiDHW / LambdaNP2
7813  -4.231 * DeltaGF()
7814  ;
7815 
7816  // Add modifications due to small variations of the SM parameters
7817  mu += cHSM * ( -2.23 * deltaaMZ()
7818  +4.23 * deltaGmu()
7819  +9.456 * deltaMz()
7820  -0.729 * deltaMh() );
7821 
7822  } else if (Pol_em == 80. && Pol_ep == 0.){
7823  mu +=
7824  +121304. * CiHbox / LambdaNP2
7825  +434952. * CiHL1_11 / LambdaNP2
7826  -3360980. * CiHe_11 / LambdaNP2
7827  +434952. * CiHL3_11 / LambdaNP2
7828  +65624.7 * CiHD / LambdaNP2
7829  +741142. * CiHB / LambdaNP2
7830  +217654. * CiHW / LambdaNP2
7831  +1046799. * CiHWB / LambdaNP2
7832  +357606. * CiDHB / LambdaNP2
7833  +4440.1 * CiDHW / LambdaNP2
7834  +0.161 * DeltaGF()
7835  ;
7836 
7837  // Add modifications due to small variations of the SM parameters
7838  mu += cHSM * ( +2.163 * deltaaMZ()
7839  -0.163 * deltaGmu()
7840  +0.671 * deltaMz()
7841  -0.729 * deltaMh() );
7842 
7843  } else if (Pol_em == -80. && Pol_ep == 0.){
7844  mu +=
7845  +121259. * CiHbox / LambdaNP2
7846  +3068356. * CiHL1_11 / LambdaNP2
7847  -292427. * CiHe_11 / LambdaNP2
7848  +3068356. * CiHL3_11 / LambdaNP2
7849  -62160.7 * CiHD / LambdaNP2
7850  -271962. * CiHB / LambdaNP2
7851  +1231171. * CiHW / LambdaNP2
7852  -206112. * CiHWB / LambdaNP2
7853  -174718. * CiDHB / LambdaNP2
7854  +296046. * CiDHW / LambdaNP2
7855  -4.053 * DeltaGF()
7856  ;
7857 
7858  // Add modifications due to small variations of the SM parameters
7859  mu += cHSM * ( -2.052 * deltaaMZ()
7860  +4.052 * deltaGmu()
7861  +9.1 * deltaMz()
7862  -0.729 * deltaMh() );
7863 
7864  } else {
7865  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
7866  }
7867 
7868  } else if (sqrt_s == 0.365) {
7869 
7870  C1 = 0.0057; // Use same as 350 GeV
7871 
7872  if (Pol_em == 80. && Pol_ep == -30.){
7873  mu +=
7874  +121270. * CiHbox / LambdaNP2
7875  +271098. * CiHL1_11 / LambdaNP2
7876  -3890169. * CiHe_11 / LambdaNP2
7877  +271098. * CiHL3_11 / LambdaNP2
7878  +74554. * CiHD / LambdaNP2
7879  +840573. * CiHB / LambdaNP2
7880  +147108. * CiHW / LambdaNP2
7881  +1160947. * CiHWB / LambdaNP2
7882  +442125. * CiDHB / LambdaNP2
7883  -15038.8 * CiDHW / LambdaNP2
7884  +0.459 * DeltaGF()
7885  ;
7886 
7887  // Add modifications due to small variations of the SM parameters
7888  mu += cHSM * ( +2.46 * deltaaMZ()
7889  -0.46 * deltaGmu()
7890  +0.029 * deltaMz()
7891  -0.664 * deltaMh() );
7892 
7893  } else if (Pol_em == -80. && Pol_ep == 30.){
7894  mu +=
7895  +121238. * CiHbox / LambdaNP2
7896  +3457848. * CiHL1_11 / LambdaNP2
7897  -177584. * CiHe_11 / LambdaNP2
7898  +3457848. * CiHL3_11 / LambdaNP2
7899  -67578.3 * CiHD / LambdaNP2
7900  -327391. * CiHB / LambdaNP2
7901  +1315671. * CiHW / LambdaNP2
7902  -259142. * CiHWB / LambdaNP2
7903  -218241. * CiDHB / LambdaNP2
7904  +346804. * CiDHW / LambdaNP2
7905  -4.231 * DeltaGF()
7906  ;
7907 
7908  // Add modifications due to small variations of the SM parameters
7909  mu += cHSM * ( -2.23 * deltaaMZ()
7910  +4.23 * deltaGmu()
7911  +9.408 * deltaMz()
7912  -0.664 * deltaMh() );
7913 
7914  } else if (Pol_em == 80. && Pol_ep == 0.){
7915  mu +=
7916  +121251. * CiHbox / LambdaNP2
7917  +472985. * CiHL1_11 / LambdaNP2
7918  -3655203. * CiHe_11 / LambdaNP2
7919  +472985. * CiHL3_11 / LambdaNP2
7920  +65559.4 * CiHD / LambdaNP2
7921  +766585. * CiHB / LambdaNP2
7922  +221202. * CiHW / LambdaNP2
7923  +1070933. * CiHWB / LambdaNP2
7924  +400293. * CiDHB / LambdaNP2
7925  +7914.02 * CiDHW / LambdaNP2
7926  +0.161 * DeltaGF()
7927  ;
7928 
7929  // Add modifications due to small variations of the SM parameters
7930  mu += cHSM * ( +2.163 * deltaaMZ()
7931  -0.163 * deltaGmu()
7932  +0.623 * deltaMz()
7933  -0.664 * deltaMh() );
7934 
7935  } else if (Pol_em == -80. && Pol_ep == 0.){
7936  mu +=
7937  +121238. * CiHbox / LambdaNP2
7938  +3336984. * CiHL1_11 / LambdaNP2
7939  -317944. * CiHe_11 / LambdaNP2
7940  +3336984. * CiHL3_11 / LambdaNP2
7941  -62188.9 * CiHD / LambdaNP2
7942  -283174. * CiHB / LambdaNP2
7943  +1271272. * CiHW / LambdaNP2
7944  -205330. * CiHWB / LambdaNP2
7945  -193153. * CiDHB / LambdaNP2
7946  +333078. * CiDHW / LambdaNP2
7947  -4.053 * DeltaGF()
7948  ;
7949 
7950  // Add modifications due to small variations of the SM parameters
7951  mu += cHSM * ( -2.052 * deltaaMZ()
7952  +4.052 * deltaGmu()
7953  +9.052 * deltaMz()
7954  -0.664 * deltaMh() );
7955 
7956  } else {
7957  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
7958  }
7959 
7960  } else if (sqrt_s == 0.380) {
7961 
7962  C1 = 0.0057; // Use same as 350 GeV
7963 
7964  if (Pol_em == 80. && Pol_ep == -30.){
7965  mu +=
7966  +121228. * CiHbox / LambdaNP2
7967  +293860. * CiHL1_11 / LambdaNP2
7968  -4216491. * CiHe_11 / LambdaNP2
7969  +293860. * CiHL3_11 / LambdaNP2
7970  +74561.4 * CiHD / LambdaNP2
7971  +866754. * CiHB / LambdaNP2
7972  +147982. * CiHW / LambdaNP2
7973  +1184912. * CiHWB / LambdaNP2
7974  +492018. * CiDHB / LambdaNP2
7975  -13596.5 * CiDHW / LambdaNP2
7976  +0.459 * DeltaGF()
7977  ;
7978 
7979  // Add modifications due to small variations of the SM parameters
7980  mu += cHSM * ( +2.46 * deltaaMZ()
7981  -0.46 * deltaGmu()
7982  -0.018 * deltaMz()
7983  -0.609 * deltaMh() );
7984 
7985  } else if (Pol_em == -80. && Pol_ep == 30.){
7986  mu +=
7987  +121226. * CiHbox / LambdaNP2
7988  +3747707. * CiHL1_11 / LambdaNP2
7989  -192650. * CiHe_11 / LambdaNP2
7990  +3747707. * CiHL3_11 / LambdaNP2
7991  -67608.3 * CiHD / LambdaNP2
7992  -339193. * CiHB / LambdaNP2
7993  +1354040. * CiHW / LambdaNP2
7994  -259321. * CiHWB / LambdaNP2
7995  -240311. * CiDHB / LambdaNP2
7996  +387710. * CiDHW / LambdaNP2
7997  -4.23 * DeltaGF()
7998  ;
7999 
8000  // Add modifications due to small variations of the SM parameters
8001  mu += cHSM * ( -2.23 * deltaaMZ()
8002  +4.23 * deltaGmu()
8003  +9.361 * deltaMz()
8004  -0.609 * deltaMh() );
8005 
8006  } else if (Pol_em == 80. && Pol_ep == 0.){
8007  mu +=
8008  +121325. * CiHbox / LambdaNP2
8009  +512707. * CiHL1_11 / LambdaNP2
8010  -3961665. * CiHe_11 / LambdaNP2
8011  +512707. * CiHL3_11 / LambdaNP2
8012  +65601.7 * CiHD / LambdaNP2
8013  +790306. * CiHB / LambdaNP2
8014  +224394. * CiHW / LambdaNP2
8015  +1093297. * CiHWB / LambdaNP2
8016  +445530. * CiDHB / LambdaNP2
8017  +11860.4 * CiDHW / LambdaNP2
8018  +0.161 * DeltaGF()
8019  ;
8020 
8021  // Add modifications due to small variations of the SM parameters
8022  mu += cHSM * ( +2.163 * deltaaMZ()
8023  -0.163 * deltaGmu()
8024  +0.576 * deltaMz()
8025  -0.609 * deltaMh() );
8026 
8027  } else if (Pol_em == -80. && Pol_ep == 0.){
8028  mu +=
8029  +121273. * CiHbox / LambdaNP2
8030  +3617032. * CiHL1_11 / LambdaNP2
8031  -344629. * CiHe_11 / LambdaNP2
8032  +3617032. * CiHL3_11 / LambdaNP2
8033  -62148.3 * CiHD / LambdaNP2
8034  -293491. * CiHB / LambdaNP2
8035  +1308558. * CiHW / LambdaNP2
8036  -204594. * CiHWB / LambdaNP2
8037  -212514. * CiDHB / LambdaNP2
8038  +372554. * CiDHW / LambdaNP2
8039  -4.053 * DeltaGF()
8040  ;
8041 
8042  // Add modifications due to small variations of the SM parameters
8043  mu += cHSM * ( -2.052 * deltaaMZ()
8044  +4.052 * deltaGmu()
8045  +9.005 * deltaMz()
8046  -0.609 * deltaMh() );
8047 
8048  } else {
8049  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
8050  }
8051 
8052  } else if (sqrt_s == 0.500) {
8053 
8054  C1 = 0.00099;
8055 
8056  if (Pol_em == 80. && Pol_ep == -30.){
8057  mu +=
8058  +121268. * CiHbox / LambdaNP2
8059  +508715. * CiHL1_11 / LambdaNP2
8060  -7299333. * CiHe_11 / LambdaNP2
8061  +508715. * CiHL3_11 / LambdaNP2
8062  +74603.6 * CiHD / LambdaNP2
8063  +1018069. * CiHB / LambdaNP2
8064  +151257. * CiHW / LambdaNP2
8065  +1323862. * CiHWB / LambdaNP2
8066  +985604. * CiDHB / LambdaNP2
8067  +8362.16 * CiDHW / LambdaNP2
8068  +0.458 * DeltaGF()
8069  ;
8070 
8071  // Add modifications due to small variations of the SM parameters
8072  mu += cHSM * ( +2.46 * deltaaMZ()
8073  -0.46 * deltaGmu()
8074  -0.319 * deltaMz()
8075  -0.351 * deltaMh() );
8076 
8077  } else if (Pol_em == -80. && Pol_ep == 30.){
8078  mu +=
8079  +121273. * CiHbox / LambdaNP2
8080  +6488707. * CiHL1_11 / LambdaNP2
8081  -332950. * CiHe_11 / LambdaNP2
8082  +6488707. * CiHL3_11 / LambdaNP2
8083  -67530.9 * CiHD / LambdaNP2
8084  -408101. * CiHB / LambdaNP2
8085  +1576859. * CiHW / LambdaNP2
8086  -260777. * CiHWB / LambdaNP2
8087  -452746. * CiDHB / LambdaNP2
8088  +796569. * CiDHW / LambdaNP2
8089  -4.231 * DeltaGF()
8090  ;
8091 
8092  // Add modifications due to small variations of the SM parameters
8093  mu += cHSM * ( -2.23 * deltaaMZ()
8094  +4.23 * deltaGmu()
8095  +9.06 * deltaMz()
8096  -0.351 * deltaMh() );
8097 
8098  } else if (Pol_em == 80. && Pol_ep == 0.){
8099  mu +=
8100  +121280. * CiHbox / LambdaNP2
8101  +887632. * CiHL1_11 / LambdaNP2
8102  -6858533. * CiHe_11 / LambdaNP2
8103  +887632. * CiHL3_11 / LambdaNP2
8104  +65606.6 * CiHD / LambdaNP2
8105  +927745. * CiHB / LambdaNP2
8106  +241619. * CiHW / LambdaNP2
8107  +1223535. * CiHWB / LambdaNP2
8108  +894441. * CiDHB / LambdaNP2
8109  +58317. * CiDHW / LambdaNP2
8110  +0.161 * DeltaGF()
8111  ;
8112 
8113  // Add modifications due to small variations of the SM parameters
8114  mu += cHSM * ( +2.163 * deltaaMZ()
8115  -0.163 * deltaGmu()
8116  +0.275 * deltaMz()
8117  -0.351 * deltaMh() );
8118 
8119  } else if (Pol_em == -80. && Pol_ep == 0.){
8120  mu +=
8121  +121268. * CiHbox / LambdaNP2
8122  +6262095. * CiHL1_11 / LambdaNP2
8123  -597046. * CiHe_11 / LambdaNP2
8124  +6262095. * CiHL3_11 / LambdaNP2
8125  -62148.8 * CiHD / LambdaNP2
8126  -353914. * CiHB / LambdaNP2
8127  +1522841. * CiHW / LambdaNP2
8128  -200684. * CiHWB / LambdaNP2
8129  -398214. * CiDHB / LambdaNP2
8130  +766821. * CiDHW / LambdaNP2
8131  -4.054 * DeltaGF()
8132  ;
8133 
8134  // Add modifications due to small variations of the SM parameters
8135  mu += cHSM * ( -2.052 * deltaaMZ()
8136  +4.052 * deltaGmu()
8137  +8.704 * deltaMz()
8138  -0.351 * deltaMh() );
8139 
8140  } else {
8141  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
8142  }
8143 
8144  } else if (sqrt_s == 1.0) {
8145 
8146  C1 = -0.0012;
8147 
8148  if (Pol_em == 80. && Pol_ep == -30.){
8149  mu +=
8150  +121236. * CiHbox / LambdaNP2
8151  +2034785. * CiHL1_11 / LambdaNP2
8152  -29195703. * CiHe_11 / LambdaNP2
8153  +2034785. * CiHL3_11 / LambdaNP2
8154  +74612.7 * CiHD / LambdaNP2
8155  +1218284. * CiHB / LambdaNP2
8156  +154779. * CiHW / LambdaNP2
8157  +1507673. * CiHWB / LambdaNP2
8158  +4701988. * CiDHB / LambdaNP2
8159  +239404. * CiDHW / LambdaNP2
8160  +0.458 * DeltaGF()
8161  ;
8162 
8163  // Add modifications due to small variations of the SM parameters
8164  mu += cHSM * ( +2.46 * deltaaMZ()
8165  -0.46 * deltaGmu()
8166  -0.745 * deltaMz()
8167  -0.092 * deltaMh() );
8168 
8169  } else if (Pol_em == -80. && Pol_ep == 30.){
8170  mu +=
8171  +121298. * CiHbox / LambdaNP2
8172  +25954994. * CiHL1_11 / LambdaNP2
8173  -1333713. * CiHe_11 / LambdaNP2
8174  +25954994. * CiHL3_11 / LambdaNP2
8175  -67536.7 * CiHD / LambdaNP2
8176  -499699. * CiHB / LambdaNP2
8177  +1872177. * CiHW / LambdaNP2
8178  -263454. * CiHWB / LambdaNP2
8179  -1999387. * CiDHB / LambdaNP2
8180  +3910434. * CiDHW / LambdaNP2
8181  -4.233 * DeltaGF()
8182  ;
8183 
8184  // Add modifications due to small variations of the SM parameters
8185  mu += cHSM * ( -2.23 * deltaaMZ()
8186  +4.23 * deltaGmu()
8187  +8.633 * deltaMz()
8188  -0.092 * deltaMh() );
8189 
8190  } else if (Pol_em == 80. && Pol_ep == -20.){
8191  mu +=
8192  +121257. * CiHbox / LambdaNP2
8193  +2475072. * CiHL1_11 / LambdaNP2
8194  -28682974. * CiHe_11 / LambdaNP2
8195  +2475072. * CiHL3_11 / LambdaNP2
8196  +72023. * CiHD / LambdaNP2
8197  +1186280. * CiHB / LambdaNP2
8198  +186435. * CiHW / LambdaNP2
8199  +1475072. * CiHWB / LambdaNP2
8200  +4578518. * CiDHB / LambdaNP2
8201  +307070. * CiDHW / LambdaNP2
8202  +0.371 * DeltaGF()
8203  ;
8204 
8205  // Add modifications due to small variations of the SM parameters
8206  mu += cHSM * ( -0.572 * deltaMz()
8207  -0.091 * deltaMh()
8208  +2.375 * deltaaMZ()
8209  -0.377 * deltaGmu() );
8210 
8211  } else if (Pol_em == -80. && Pol_ep == 20.){
8212  mu +=
8213  +121306. * CiHbox / LambdaNP2
8214  +25696973. * CiHL1_11 / LambdaNP2
8215  -1634825. * CiHe_11 / LambdaNP2
8216  +25696973. * CiHL3_11 / LambdaNP2
8217  -65976.8 * CiHD / LambdaNP2
8218  -480973. * CiHB / LambdaNP2
8219  +1853631. * CiHW / LambdaNP2
8220  -244288. * CiHWB / LambdaNP2
8221  -1927204. * CiDHB / LambdaNP2
8222  +3870798. * CiDHW / LambdaNP2
8223  -4.182 * DeltaGF()
8224  ;
8225 
8226  // Add modifications due to small variations of the SM parameters
8227  mu += cHSM * ( +8.536 * deltaMz()
8228  -0.09 * deltaMh()
8229  -2.178 * deltaaMZ()
8230  +4.178 * deltaGmu() );
8231 
8232  } else if (Pol_em == 80. && Pol_ep == 0.){
8233  mu +=
8234  +121307. * CiHbox / LambdaNP2
8235  +3550656. * CiHL1_11 / LambdaNP2
8236  -27432206. * CiHe_11 / LambdaNP2
8237  +3550656. * CiHL3_11 / LambdaNP2
8238  +65607.4 * CiHD / LambdaNP2
8239  +1109435. * CiHB / LambdaNP2
8240  +263679. * CiHW / LambdaNP2
8241  +1395519. * CiHWB / LambdaNP2
8242  +4277336. * CiDHB / LambdaNP2
8243  +472106. * CiDHW / LambdaNP2
8244  +0.159 * DeltaGF()
8245  ;
8246 
8247  // Add modifications due to small variations of the SM parameters
8248  mu += cHSM * ( +2.163 * deltaaMZ()
8249  -0.163 * deltaGmu()
8250  -0.151 * deltaMz()
8251  -0.092 * deltaMh() );
8252 
8253  } else if (Pol_em == -80. && Pol_ep == 0.){
8254  mu +=
8255  +121327. * CiHbox / LambdaNP2
8256  +25048839. * CiHL1_11 / LambdaNP2
8257  -2390358. * CiHe_11 / LambdaNP2
8258  +25048839. * CiHL3_11 / LambdaNP2
8259  -62132.7 * CiHD / LambdaNP2
8260  -434824. * CiHB / LambdaNP2
8261  +1807095. * CiHW / LambdaNP2
8262  -196264. * CiHWB / LambdaNP2
8263  -1746222. * CiDHB / LambdaNP2
8264  +3771341. * CiDHW / LambdaNP2
8265  -4.056 * DeltaGF()
8266  ;
8267 
8268  // Add modifications due to small variations of the SM parameters
8269  mu += cHSM * ( -2.052 * deltaaMZ()
8270  +4.052 * deltaGmu()
8271  +8.278 * deltaMz()
8272  -0.092 * deltaMh() );
8273 
8274  } else {
8275  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
8276  }
8277 
8278  } else if (sqrt_s == 1.4) {
8279 
8280  C1 = -0.0011;
8281 
8282  if (Pol_em == 80. && Pol_ep == -30.){
8283  mu +=
8284  +121277. * CiHbox / LambdaNP2
8285  +3988231. * CiHL1_11 / LambdaNP2
8286  -57226150. * CiHe_11 / LambdaNP2
8287  +3988231. * CiHL3_11 / LambdaNP2
8288  +74608.5 * CiHD / LambdaNP2
8289  +1256970. * CiHB / LambdaNP2
8290  +155358. * CiHW / LambdaNP2
8291  +1542655. * CiHWB / LambdaNP2
8292  +9506894. * CiDHB / LambdaNP2
8293  +553431. * CiDHW / LambdaNP2
8294  +0.457 * DeltaGF()
8295  ;
8296 
8297  // Add modifications due to small variations of the SM parameters
8298  mu += cHSM * ( +2.46 * deltaaMZ()
8299  -0.46 * deltaGmu()
8300  -0.828 * deltaMz()
8301  -0.047 * deltaMh() );
8302 
8303  } else if (Pol_em == -80. && Pol_ep == 30.){
8304  mu +=
8305  +121314. * CiHbox / LambdaNP2
8306  +50871646. * CiHL1_11 / LambdaNP2
8307  -2614134. * CiHe_11 / LambdaNP2
8308  +50871646. * CiHL3_11 / LambdaNP2
8309  -67535.5 * CiHD / LambdaNP2
8310  -516385. * CiHB / LambdaNP2
8311  +1928805. * CiHW / LambdaNP2
8312  -264072. * CiHWB / LambdaNP2
8313  -3989947. * CiDHB / LambdaNP2
8314  +7948308. * CiDHW / LambdaNP2
8315  -4.233 * DeltaGF()
8316  ;
8317 
8318  // Add modifications due to small variations of the SM parameters
8319  mu += cHSM * ( -2.23 * deltaaMZ()
8320  +4.23 * deltaGmu()
8321  +8.55 * deltaMz()
8322  -0.047 * deltaMh() );
8323 
8324  } else if (Pol_em == 80. && Pol_ep == 0.){
8325  mu +=
8326  +121250. * CiHbox / LambdaNP2
8327  +6958750. * CiHL1_11 / LambdaNP2
8328  -53762500. * CiHe_11 / LambdaNP2
8329  +6958750. * CiHL3_11 / LambdaNP2
8330  +65589.3 * CiHD / LambdaNP2
8331  +1144464. * CiHB / LambdaNP2
8332  +267732. * CiHW / LambdaNP2
8333  +1428214. * CiHWB / LambdaNP2
8334  +8650536. * CiDHB / LambdaNP2
8335  +1021964. * CiDHW / LambdaNP2
8336  +0.16 * DeltaGF()
8337  ;
8338 
8339  // Add modifications due to small variations of the SM parameters
8340  mu += cHSM * ( +2.163 * deltaaMZ()
8341  -0.163 * deltaGmu()
8342  -0.234 * deltaMz()
8343  -0.047 * deltaMh() );
8344 
8345  } else if (Pol_em == -80. && Pol_ep == 0.){
8346  mu +=
8347  +121278. * CiHbox / LambdaNP2
8348  +49094486. * CiHL1_11 / LambdaNP2
8349  -4685522. * CiHe_11 / LambdaNP2
8350  +49094486. * CiHL3_11 / LambdaNP2
8351  -62150.9 * CiHD / LambdaNP2
8352  -450090. * CiHB / LambdaNP2
8353  +1861602. * CiHW / LambdaNP2
8354  -195621. * CiHWB / LambdaNP2
8355  -3478338. * CiDHB / LambdaNP2
8356  +7668095. * CiDHW / LambdaNP2
8357  -4.055 * DeltaGF()
8358  ;
8359 
8360  // Add modifications due to small variations of the SM parameters
8361  mu += cHSM * ( -2.052 * deltaaMZ()
8362  +4.052 * deltaGmu()
8363  +8.195 * deltaMz()
8364  -0.047 * deltaMh() );
8365 
8366  } else {
8367  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
8368  }
8369 
8370  } else if (sqrt_s == 1.5) {
8371 
8372  C1 = -0.0011;// Use the same as 1400 GeV
8373 
8374  if (Pol_em == 80. && Pol_ep == -30.){
8375  mu +=
8376  +121268. * CiHbox / LambdaNP2
8377  +4578315. * CiHL1_11 / LambdaNP2
8378  -65691823. * CiHe_11 / LambdaNP2
8379  +4578315. * CiHL3_11 / LambdaNP2
8380  +74595.2 * CiHD / LambdaNP2
8381  +1262261. * CiHB / LambdaNP2
8382  +155435. * CiHW / LambdaNP2
8383  +1547379. * CiHWB / LambdaNP2
8384  +10961322. * CiDHB / LambdaNP2
8385  +649157. * CiDHW / LambdaNP2
8386  +0.457 * DeltaGF()
8387  ;
8388 
8389  // Add modifications due to small variations of the SM parameters
8390  mu += cHSM * ( +2.46 * deltaaMZ()
8391  -0.46 * deltaGmu()
8392  -0.84 * deltaMz()
8393  -0.041 * deltaMh() );
8394 
8395  } else if (Pol_em == -80. && Pol_ep == 30.){
8396  mu +=
8397  +121277. * CiHbox / LambdaNP2
8398  +58398883. * CiHL1_11 / LambdaNP2
8399  -3000385. * CiHe_11 / LambdaNP2
8400  +58398883. * CiHL3_11 / LambdaNP2
8401  -67535.8 * CiHD / LambdaNP2
8402  -518798. * CiHB / LambdaNP2
8403  +1936613. * CiHW / LambdaNP2
8404  -264171. * CiHWB / LambdaNP2
8405  -4590136. * CiDHB / LambdaNP2
8406  +9169803. * CiDHW / LambdaNP2
8407  -4.233 * DeltaGF()
8408  ;
8409 
8410  // Add modifications due to small variations of the SM parameters
8411  mu += cHSM * ( -2.23 * deltaaMZ()
8412  +4.23 * deltaGmu()
8413  +8.539 * deltaMz()
8414  -0.041 * deltaMh() );
8415 
8416  } else if (Pol_em == 80. && Pol_ep == 0.){
8417  mu +=
8418  +121289. * CiHbox / LambdaNP2
8419  +7988570. * CiHL1_11 / LambdaNP2
8420  -61718691. * CiHe_11 / LambdaNP2
8421  +7988570. * CiHL3_11 / LambdaNP2
8422  +65599. * CiHD / LambdaNP2
8423  +1149083. * CiHB / LambdaNP2
8424  +268317. * CiHW / LambdaNP2
8425  +1432777. * CiHWB / LambdaNP2
8426  +9972576. * CiDHB / LambdaNP2
8427  +1188554. * CiDHW / LambdaNP2
8428  +0.16 * DeltaGF()
8429  ;
8430 
8431  // Add modifications due to small variations of the SM parameters
8432  mu += cHSM * ( +2.163 * deltaaMZ()
8433  -0.163 * deltaGmu()
8434  -0.246 * deltaMz()
8435  -0.041 * deltaMh() );
8436 
8437  } else if (Pol_em == -80. && Pol_ep == 0.){
8438  mu +=
8439  +121259. * CiHbox / LambdaNP2
8440  +56356946. * CiHL1_11 / LambdaNP2
8441  -5378233. * CiHe_11 / LambdaNP2
8442  +56356946. * CiHL3_11 / LambdaNP2
8443  -62168.7 * CiHD / LambdaNP2
8444  -452149. * CiHB / LambdaNP2
8445  +1869136. * CiHW / LambdaNP2
8446  -195562. * CiHWB / LambdaNP2
8447  -4000306. * CiDHB / LambdaNP2
8448  +8846432. * CiDHW / LambdaNP2
8449  -4.055 * DeltaGF()
8450  ;
8451 
8452  // Add modifications due to small variations of the SM parameters
8453  mu += cHSM * ( -2.052 * deltaaMZ()
8454  +4.052 * deltaGmu()
8455  +8.183 * deltaMz()
8456  -0.041 * deltaMh() );
8457 
8458  } else {
8459  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
8460  }
8461 
8462  } else if (sqrt_s == 3.0) {
8463 
8464  C1 = -0.00054;
8465 
8466  if (Pol_em == 80. && Pol_ep == -30.){
8467  mu +=
8468  +121320. * CiHbox / LambdaNP2
8469  +18314161. * CiHL1_11 / LambdaNP2
8470  -262773345. * CiHe_11 / LambdaNP2
8471  +18314161. * CiHL3_11 / LambdaNP2
8472  +74663.6 * CiHD / LambdaNP2
8473  +1289569. * CiHB / LambdaNP2
8474  +155612. * CiHW / LambdaNP2
8475  +1572580. * CiHWB / LambdaNP2
8476  +44806408. * CiDHB / LambdaNP2
8477  +2877519. * CiDHW / LambdaNP2
8478  +0.456 * DeltaGF()
8479  ;
8480 
8481  // Add modifications due to small variations of the SM parameters
8482  mu += cHSM * ( +2.46 * deltaaMZ()
8483  -0.46 * deltaGmu()
8484  -0.899 * deltaMz()
8485  -0.01 * deltaMh() );
8486 
8487  } else if (Pol_em == -80. && Pol_ep == 30.){
8488  mu +=
8489  +121305. * CiHbox / LambdaNP2
8490  +233598342. * CiHL1_11 / LambdaNP2
8491  -12002450. * CiHe_11 / LambdaNP2
8492  +233598342. * CiHL3_11 / LambdaNP2
8493  -67507.7 * CiHD / LambdaNP2
8494  -531387. * CiHB / LambdaNP2
8495  +1976750. * CiHW / LambdaNP2
8496  -264661. * CiHWB / LambdaNP2
8497  -18587969. * CiDHB / LambdaNP2
8498  +37618569. * CiDHW / LambdaNP2
8499  -4.233 * DeltaGF()
8500  ;
8501 
8502  // Add modifications due to small variations of the SM parameters
8503  mu += cHSM * ( -2.23 * deltaaMZ()
8504  +4.23 * deltaGmu()
8505  +8.48 * deltaMz()
8506  -0.01 * deltaMh() );
8507 
8508  } else if (Pol_em == 80. && Pol_ep == 0.){
8509  mu +=
8510  +121225. * CiHbox / LambdaNP2
8511  +31953446. * CiHL1_11 / LambdaNP2
8512  -246870182. * CiHe_11 / LambdaNP2
8513  +31953446. * CiHL3_11 / LambdaNP2
8514  +65576.5 * CiHD / LambdaNP2
8515  +1173703. * CiHB / LambdaNP2
8516  +270983. * CiHW / LambdaNP2
8517  +1456032. * CiHWB / LambdaNP2
8518  +40783748. * CiDHB / LambdaNP2
8519  +5077924. * CiDHW / LambdaNP2
8520  +0.16 * DeltaGF()
8521  ;
8522 
8523  // Add modifications due to small variations of the SM parameters
8524  mu += cHSM * ( +2.163 * deltaaMZ()
8525  -0.163 * deltaGmu()
8526  -0.305 * deltaMz()
8527  -0.01 * deltaMh() );
8528 
8529  } else if (Pol_em == -80. && Pol_ep == 0.){
8530  mu +=
8531  +121248. * CiHbox / LambdaNP2
8532  +225427310. * CiHL1_11 / LambdaNP2
8533  -21505526. * CiHe_11 / LambdaNP2
8534  +225427310. * CiHL3_11 / LambdaNP2
8535  -62193.4 * CiHD / LambdaNP2
8536  -463403. * CiHB / LambdaNP2
8537  +1907593. * CiHW / LambdaNP2
8538  -195017. * CiHWB / LambdaNP2
8539  -16188019. * CiDHB / LambdaNP2
8540  +36299719. * CiDHW / LambdaNP2
8541  -4.054 * DeltaGF()
8542  ;
8543 
8544  // Add modifications due to small variations of the SM parameters
8545  mu += cHSM * ( -2.052 * deltaaMZ()
8546  +4.052 * deltaGmu()
8547  +8.124 * deltaMz()
8548  -0.01 * deltaMh() );
8549 
8550  } else {
8551  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
8552  }
8553 
8554  } else
8555  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
8556 
8557  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
8558  mu += eeeZHint + eeeZHpar;
8559 
8560 // Linear contribution from Higgs self-coupling
8561  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
8562 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
8564 
8565  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
8566 
8567  return mu;
8568 }

◆ mueeZllH()

double NPSMEFTd6::mueeZllH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\)

Reimplemented from NPbase.

Definition at line 7541 of file NPSMEFTd6.cpp.

7542 {
7543 
7544 // The signal strength eeZH
7545  double mu = mueeZH(sqrt_s);
7546 
7547 // The (relative) linear correction to the Z>ll BR
7548  double deltaBRratio;
7549 
7550  deltaBRratio = deltaGamma_Zf(leptons[ELECTRON])
7551  + deltaGamma_Zf(leptons[MU]);
7552 
7553  deltaBRratio = deltaBRratio /
7555 
7556  deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
7557 
7558  return mu + deltaBRratio;
7559 }

◆ mueeZllHPol()

double NPSMEFTd6::mueeZllHPol ( const double  sqrt_s,
const double  Pol_em,
const double  Pol_ep 
) const
virtual

The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively
Returns
\(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\)

Reimplemented from NPbase.

Definition at line 8570 of file NPSMEFTd6.cpp.

8571 {
8572 
8573 // The signal strength eeZH
8574  double mu = mueeZHPol(sqrt_s, Pol_em, Pol_ep);
8575 
8576 // The (relative) linear correction to the Z>ll BR
8577  double deltaBRratio;
8578 
8579  deltaBRratio = deltaGamma_Zf(leptons[ELECTRON])
8580  + deltaGamma_Zf(leptons[MU]);
8581 
8582  deltaBRratio = deltaBRratio /
8584 
8585  deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
8586 
8587  return mu + deltaBRratio;
8588 }

◆ mueeZqqH()

double NPSMEFTd6::mueeZqqH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{eeZH, Z \to q \bar{q}}\)

Reimplemented from NPbase.

Definition at line 7561 of file NPSMEFTd6.cpp.

7562 {
7563 
7564 // The signal strength eeZH
7565  double mu = mueeZH(sqrt_s);
7566 
7567 // The (relative) linear correction to the Z>qq BR
7568  double deltaBRratio;
7569 
7570  deltaBRratio = deltaGamma_Zf(quarks[UP])
7575 
7576  deltaBRratio = deltaBRratio /
7579  + trueSM.GammaZ(quarks[BOTTOM]));
7580 
7581  deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
7582 
7583  return mu + deltaBRratio;
7584 }

◆ mueeZqqHPol()

double NPSMEFTd6::mueeZqqHPol ( const double  sqrt_s,
const double  Pol_em,
const double  Pol_ep 
) const
virtual

The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively
Returns
\(\mu_{eeZH, Z \to q \bar{q}}\)

Reimplemented from NPbase.

Definition at line 8590 of file NPSMEFTd6.cpp.

8591 {
8592 
8593 // The signal strength eeZH
8594  double mu = mueeZHPol(sqrt_s, Pol_em, Pol_ep);
8595 
8596 // The (relative) linear correction to the Z>qq BR
8597  double deltaBRratio;
8598 
8599  deltaBRratio = deltaGamma_Zf(quarks[UP])
8604 
8605  deltaBRratio = deltaBRratio /
8608  + trueSM.GammaZ(quarks[BOTTOM]));
8609 
8610  deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
8611 
8612  return mu + deltaBRratio;
8613 }

◆ muepWBF()

double NPSMEFTd6::muepWBF ( const double  sqrt_s) const
virtual

The ratio \(\mu_{epWBF}\) between the \( e^{-} p\to \nu j H \) production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{epWBF}\)

Reimplemented from NPbase.

Definition at line 6658 of file NPSMEFTd6.cpp.

6659 {
6660  double mu = 1.0;
6661 
6662  if (sqrt_s == 1.3) {
6663 
6664  mu +=
6665  +121790. * CiHbox / LambdaNP2
6666  -161604. * CiHL3_11 / LambdaNP2
6667  -161282. * CiHQ3_11 / LambdaNP2
6668  -203141. * CiHD / LambdaNP2
6669  -88171.6 * CiHW / LambdaNP2
6670  -377218. * CiHWB / LambdaNP2
6671  -37738.9 * CiDHW / LambdaNP2
6672  -4.676 * DeltaGF()
6673  -4.916 * deltaMwd6()
6674  ;
6675 
6676 // if (FlagQuadraticTerms) {
6677  //Add contributions that are quadratic in the effective coefficients
6678 
6679 // }
6680 
6681  } else if (sqrt_s == 1.8) {
6682 
6683  mu +=
6684  +121867. * CiHbox / LambdaNP2
6685  -182643. * CiHL3_11 / LambdaNP2
6686  -181961. * CiHQ3_11 / LambdaNP2
6687  -202400. * CiHD / LambdaNP2
6688  -78295.8 * CiHW / LambdaNP2
6689  -377193. * CiHWB / LambdaNP2
6690  -45757.3 * CiDHW / LambdaNP2
6691  -4.672 * DeltaGF()
6692  -4.637 * deltaMwd6()
6693  ;
6694 
6695 // if (FlagQuadraticTerms) {
6696  //Add contributions that are quadratic in the effective coefficients
6697 
6698 // }
6699 
6700  } else if (sqrt_s == 3.5) {
6701 
6702  mu +=
6703  +121250. * CiHbox / LambdaNP2
6704  -216885. * CiHL3_11 / LambdaNP2
6705  -218544. * CiHQ3_11 / LambdaNP2
6706  -202390. * CiHD / LambdaNP2
6707  -64783.2 * CiHW / LambdaNP2
6708  -377727. * CiHWB / LambdaNP2
6709  -60431.2 * CiDHW / LambdaNP2
6710  -4.688 * DeltaGF()
6711  -4.573 * deltaMwd6()
6712  ;
6713 
6714 // if (FlagQuadraticTerms) {
6715  //Add contributions that are quadratic in the effective coefficients
6716 
6717 // }
6718 
6719  } else if (sqrt_s == 5.0) {
6720 
6721  mu +=
6722  +119662. * CiHbox / LambdaNP2
6723  -237868. * CiHL3_11 / LambdaNP2
6724  -236470. * CiHQ3_11 / LambdaNP2
6725  -203294. * CiHD / LambdaNP2
6726  -60911. * CiHW / LambdaNP2
6727  -378045. * CiHWB / LambdaNP2
6728  -67483.7 * CiDHW / LambdaNP2
6729  -4.667 * DeltaGF()
6730  -4.437 * deltaMwd6()
6731  ;
6732 
6733 // if (FlagQuadraticTerms) {
6734  //Add contributions that are quadratic in the effective coefficients
6735 
6736 // }
6737 
6738  } else
6739  throw std::runtime_error("Bad argument in NPSMEFTd6::muepWBF()");
6740 
6741  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
6742  mu += eepWBFint + eepWBFpar;
6743 
6744  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
6745 
6746  return mu;
6747 }

◆ muepZBF()

double NPSMEFTd6::muepZBF ( const double  sqrt_s) const
virtual

The ratio \(\mu_{epZBF}\) between the \( e^{-} p\to e^{-} j H \) production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{epZBF}\)

Reimplemented from NPbase.

Definition at line 6749 of file NPSMEFTd6.cpp.

6750 {
6751  double mu = 1.0;
6752 
6753  if (sqrt_s == 1.3) {
6754 
6755  mu +=
6756  +121280. * CiHbox / LambdaNP2
6757  -152367. * CiHL1_11 / LambdaNP2
6758  +32200. * CiHQ1_11 / LambdaNP2
6759  +124934. * CiHe_11 / LambdaNP2
6760  -42209.5 * CiHu_11 / LambdaNP2
6761  +12445.7 * CiHd_11 / LambdaNP2
6762  -152367. * CiHL3_11 / LambdaNP2
6763  -165343. * CiHQ3_11 / LambdaNP2
6764  -173922. * CiHD / LambdaNP2
6765  -34636.2 * CiHB / LambdaNP2
6766  -121438. * CiHW / LambdaNP2
6767  -74939.1 * CiHWB / LambdaNP2
6768  -5454.93 * CiDHB / LambdaNP2
6769  -39349.6 * CiDHW / LambdaNP2
6770  -3.719 * DeltaGF()
6771  ;
6772 
6773 // if (FlagQuadraticTerms) {
6774  //Add contributions that are quadratic in the effective coefficients
6775 
6776 // }
6777 
6778  } else if (sqrt_s == 1.8) {
6779 
6780  mu +=
6781  +120218. * CiHbox / LambdaNP2
6782  -173566. * CiHL1_11 / LambdaNP2
6783  +26307.1 * CiHQ1_11 / LambdaNP2
6784  +142600. * CiHe_11 / LambdaNP2
6785  -47449. * CiHu_11 / LambdaNP2
6786  +14356.2 * CiHd_11 / LambdaNP2
6787  -173566. * CiHL3_11 / LambdaNP2
6788  -188606. * CiHQ3_11 / LambdaNP2
6789  -174301. * CiHD / LambdaNP2
6790  -19800. * CiHB / LambdaNP2
6791  -103254. * CiHW / LambdaNP2
6792  -89049.2 * CiHWB / LambdaNP2
6793  -8304.85 * CiDHB / LambdaNP2
6794  -48942.9 * CiDHW / LambdaNP2
6795  -3.714 * DeltaGF()
6796  ;
6797 
6798 // if (FlagQuadraticTerms) {
6799  //Add contributions that are quadratic in the effective coefficients
6800 
6801 // }
6802 
6803  } else if (sqrt_s == 3.5) {
6804 
6805  mu +=
6806  +123119. * CiHbox / LambdaNP2
6807  -206981. * CiHL1_11 / LambdaNP2
6808  +18620.9 * CiHQ1_11 / LambdaNP2
6809  +177706. * CiHe_11 / LambdaNP2
6810  -53822. * CiHu_11 / LambdaNP2
6811  +20491.5 * CiHd_11 / LambdaNP2
6812  -206981. * CiHL3_11 / LambdaNP2
6813  -227549. * CiHQ3_11 / LambdaNP2
6814  -172298. * CiHD / LambdaNP2
6815  -6887.17 * CiHB / LambdaNP2
6816  -79245. * CiHW / LambdaNP2
6817  -103223. * CiHWB / LambdaNP2
6818  -9863.11 * CiDHB / LambdaNP2
6819  -61304.3 * CiDHW / LambdaNP2
6820  -3.721 * DeltaGF()
6821  ;
6822 
6823 // if (FlagQuadraticTerms) {
6824  //Add contributions that are quadratic in the effective coefficients
6825 
6826 // }
6827 
6828  } else if (sqrt_s == 5.0) {
6829 
6830  mu +=
6831  +121709. * CiHbox / LambdaNP2
6832  -225267. * CiHL1_11 / LambdaNP2
6833  +13471.8 * CiHQ1_11 / LambdaNP2
6834  +193542. * CiHe_11 / LambdaNP2
6835  -57640.9 * CiHu_11 / LambdaNP2
6836  +22573. * CiHd_11 / LambdaNP2
6837  -225267. * CiHL3_11 / LambdaNP2
6838  -247738. * CiHQ3_11 / LambdaNP2
6839  -172768. * CiHD / LambdaNP2
6840  -4524.89 * CiHB / LambdaNP2
6841  -71935.4 * CiHW / LambdaNP2
6842  -104998. * CiHWB / LambdaNP2
6843  -11877.8 * CiDHB / LambdaNP2
6844  -69467.3 * CiDHW / LambdaNP2
6845  -3.71 * DeltaGF()
6846  ;
6847 
6848 // if (FlagQuadraticTerms) {
6849  //Add contributions that are quadratic in the effective coefficients
6850 
6851 // }
6852 
6853  } else
6854  throw std::runtime_error("Bad argument in NPSMEFTd6::muepZBF()");
6855 
6856  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
6857  mu += eepZBFint + eepZBFpar;
6858 
6859  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
6860 
6861  return mu;
6862 }

◆ muggH()

double NPSMEFTd6::muggH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH}\)

Reimplemented from NPbase.

Definition at line 3299 of file NPSMEFTd6.cpp.

3300 {
3301 
3302  double C1 = 0.0066; //It seems to be independent of energy
3303 
3304  double m_t = mtpole;
3305  //doulbe m_t = quarks[TOP].getMass();
3306  double m_b = quarks[BOTTOM].getMass();
3307  double m_c = quarks[CHARM].getMass();
3308 
3309  /* L_eff_SM = (G_eff_t_SM + G_eff_b_SM)*hGG */
3310  gslpp::complex G_eff_t_SM = AlsMz / 16.0 / M_PI / v() * AH_f(4.0 * m_t * m_t / mHl / mHl);
3311  gslpp::complex G_eff_b_SM = AlsMz / 16.0 / M_PI / v() * AH_f(4.0 * m_b * m_b / mHl / mHl);
3312  gslpp::complex G_eff_c_SM = AlsMz / 16.0 / M_PI / v() * AH_f(4.0 * m_c * m_c / mHl / mHl);
3313  gslpp::complex G_eff_SM = G_eff_t_SM + G_eff_b_SM + G_eff_c_SM;
3314 
3315  //double sigma_tt_SM = trueSM.computeSigmaggH_tt(sqrt_s);
3316  //double sigma_bb_SM = trueSM.computeSigmaggH_bb(sqrt_s);
3317  //double sigma_tb_SM = trueSM.computeSigmaggH_tb(sqrt_s);
3318  //gslpp::complex tmp = (2.0 * dKappa_t * sigma_tt_SM
3319  // + 2.0 * dKappa_b * sigma_bb_SM
3320  // + (dKappa_t + dKappa_b) * sigma_tb_SM)
3321  // / (sigma_tt_SM + sigma_bb_SM + sigma_tb_SM);
3322 
3323  gslpp::complex dKappa_t = cLHd6 * deltaG_hff(quarks[TOP]) / (-m_t / v());
3324  gslpp::complex dKappa_b = cLHd6 * deltaG_hff(quarks[BOTTOM]) / (-m_b / v());
3325  gslpp::complex dKappa_c = cLHd6 * deltaG_hff(quarks[CHARM]) / (-m_c / v());
3326 
3327  gslpp::complex tmpHG = CHG / v() * v2_over_LambdaNP2 / G_eff_SM;
3328  gslpp::complex tmpt = G_eff_t_SM * dKappa_t / G_eff_SM;
3329  gslpp::complex tmpb = G_eff_b_SM * dKappa_b / G_eff_SM;
3330  gslpp::complex tmpc = G_eff_c_SM * dKappa_c / G_eff_SM;
3331 
3332  double mu = (1.0 + 2.0 * ( tmpt.real() + tmpb.real() + tmpc.real() + tmpHG.real() ) );
3333 
3334 // Linear contribution from Higgs self-coupling
3335  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
3336 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
3338 
3339  if (FlagQuadraticTerms) {
3340  //Add contributions that are quadratic in the effective coefficients
3341  gslpp::complex tmp2 = tmpt +tmpb +tmpc + tmpHG;
3342 
3343  mu += tmp2.abs2();
3344 
3345  }
3346 
3347  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
3348  mu += eggFint + eggFpar;
3349 
3350  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
3351 
3352  return mu;
3353 }

◆ muggHbb()

double NPSMEFTd6::muggHbb ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,bb}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,bb}\)

Reimplemented from NPbase.

Definition at line 12822 of file NPSMEFTd6.cpp.

12823 {
12824  return muggH(sqrt_s) * BrHbbRatio();
12825 
12826 }

◆ muggHgaga()

double NPSMEFTd6::muggHgaga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 12534 of file NPSMEFTd6.cpp.

12535 {
12536  return muggH(sqrt_s) * BrHgagaRatio();
12537 
12538 }

◆ muggHH()

double NPSMEFTd6::muggHH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggHH}\) between the gluon-gluon fusion di-Higgs production cross-section in the current model and in the Standard Model. (From arXiv: 1502.00539 [hpe-ph].)

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggHH}\)

Reimplemented from NPbase.

Definition at line 3355 of file NPSMEFTd6.cpp.

3356 {
3357  double mu = 1.0;
3358  double A1HH = 0.0, A2HH = 0.0, A3HH = 0.0, A4HH = 0.0, A5HH = 0.0;
3359  double A6HH = 0.0, A7HH = 0.0, A8HH = 0.0, A9HH = 0.0, A10HH = 0.0;
3360  double A11HH = 0.0, A12HH = 0.0, A13HH = 0.0, A14HH = 0.0, A15HH = 0.0;
3361  double ct,c2t,c3,cg,c2g;
3362 
3363  if (sqrt_s == 14.0) {
3364 
3365  // From the cut-based analysis. Table IV
3366 
3367  A1HH = 1.70;
3368  A2HH = 10.7;
3369  A3HH = 0.117;
3370  A4HH = 6.11;
3371  A5HH = 217.0;
3372  A6HH = -7.56;
3373  A7HH = -0.819;
3374  A8HH = 1.95;
3375  A9HH = 10.90;
3376  A10HH = 51.6;
3377  A11HH = -3.86;
3378  A12HH = -12.5;
3379  A13HH = 1.46;
3380  A14HH = 5.49;
3381  A15HH = 58.4;
3382 
3383  } else if (sqrt_s == 100.0) {
3384 
3385  // From the cut-based analysis. Table IV
3386 
3387  A1HH = 1.59;
3388  A2HH = 12.8;
3389  A3HH = 0.090;
3390  A4HH = 5.2;
3391  A5HH = 358.0;
3392  A6HH = -7.66;
3393  A7HH = -0.681;
3394  A8HH = 1.83;
3395  A9HH = 9.25;
3396  A10HH = 51.2;
3397  A11HH = -2.61;
3398  A12HH = -7.35;
3399  A13HH = 1.03;
3400  A14HH = 4.65;
3401  A15HH = 65.5;
3402 
3403  } else
3404  throw std::runtime_error("Bad argument in NPSMEFTd6::muggHH()");
3405 
3406  ct= 1.0 - 0.5 * DeltaGF() + delta_h - v() * CiuH_33r * v2_over_LambdaNP2 / sqrt(2.0)/ mtpole;
3407  c2t = delta_h - 3.0 *v() * CiuH_33r * v2_over_LambdaNP2 / 2.0 /sqrt(2.0)/ mtpole;
3408  c3 = 1.0 + deltaG_hhhRatio();
3409  cg = M_PI * CHG * v2_over_LambdaNP2 / AlsMz;
3410  c2g = cg;
3411 
3412 // In the SM the Eq. returns 0.999. Fix that small offset by adding 0.0010
3413  mu = 0.0010 + A1HH*ct*ct*ct*ct +
3414  A2HH*c2t*c2t +
3415  A3HH*ct*ct*c3*c3 +
3416  A4HH*cg*cg*c3*c3 +
3417  A5HH*c2g*c2g +
3418  A6HH*c2t*ct*ct +
3419  A7HH*ct*ct*ct*c3 +
3420  A8HH*c2t*ct*c3 +
3421  A9HH*c2t*cg*c3 +
3422  A10HH*c2t*c2g +
3423  A11HH*ct*ct*cg*c3 +
3424  A12HH*ct*ct*c2g +
3425  A13HH*ct*c3*c3*cg +
3426  A14HH*ct*c3*c2g +
3427  A15HH*cg*c3*c2g;
3428 
3429  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
3430 
3431  return mu;
3432 }

◆ muggHmumu()

double NPSMEFTd6::muggHmumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,\mu\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,\mu\mu}\)

Reimplemented from NPbase.

Definition at line 12750 of file NPSMEFTd6.cpp.

12751 {
12752  return muggH(sqrt_s) * BrHmumuRatio();
12753 
12754 }

◆ muggHpttH()

double NPSMEFTd6::muggHpttH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH+ttH}\) between the sum of gluon-gluon fusion and t-tbar-Higgs associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH+ttH}\)

Reimplemented from NPbase.

Definition at line 8991 of file NPSMEFTd6.cpp.

8992 {
8993  double sigmaggH_SM = computeSigmaggH(sqrt_s);
8994  double sigmattH_SM = computeSigmattH(sqrt_s);
8995  double sigmaggH = muggH(sqrt_s) * sigmaggH_SM;
8996  double sigmattH = muttH(sqrt_s) * sigmattH_SM;
8997 
8998  double mu = ((sigmaggH + sigmattH) / (sigmaggH_SM + sigmattH_SM));
8999 
9000  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
9001 
9002  return mu;
9003 }

◆ muggHtautau()

double NPSMEFTd6::muggHtautau ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,\tau\tau}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,\tau\tau}\)

Reimplemented from NPbase.

Definition at line 12786 of file NPSMEFTd6.cpp.

12787 {
12788  return muggH(sqrt_s) * BrHtautauRatio();
12789 
12790 }

◆ muggHWW()

double NPSMEFTd6::muggHWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,WW}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,WW}\)

Reimplemented from NPbase.

Definition at line 12678 of file NPSMEFTd6.cpp.

12679 {
12680  return muggH(sqrt_s) * BrHWWRatio();
12681 
12682 }

◆ muggHWW2l2v()

double NPSMEFTd6::muggHWW2l2v ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,WW\to 2l2\nu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,WW\to 2l2\nu}\)

Reimplemented from NPbase.

Definition at line 12714 of file NPSMEFTd6.cpp.

12715 {
12716  return muggH(sqrt_s) * BrHWW2l2vRatio();
12717 
12718 }

◆ muggHZga()

double NPSMEFTd6::muggHZga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,Z\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,Z\gamma}\)

Reimplemented from NPbase.

Definition at line 12570 of file NPSMEFTd6.cpp.

12571 {
12572  return muggH(sqrt_s) * BrHZgaRatio();
12573 
12574 }

◆ muggHZZ()

double NPSMEFTd6::muggHZZ ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,ZZ}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,ZZ}\)

Reimplemented from NPbase.

Definition at line 12606 of file NPSMEFTd6.cpp.

12607 {
12608  return muggH(sqrt_s) * BrHZZRatio();
12609 
12610 }

◆ muggHZZ4l()

double NPSMEFTd6::muggHZZ4l ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,ZZ\to 4l}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,ZZ\to 4l}\)

Reimplemented from NPbase.

Definition at line 12642 of file NPSMEFTd6.cpp.

12643 {
12644  return muggH(sqrt_s) * BrHZZ4lRatio();
12645 
12646 }

◆ mummH()

double NPSMEFTd6::mummH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{\mu\mu H}\) between the \(\sigma(\mu \mu \to H)}\) production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{\mu\mu H}\)

Reimplemented from NPbase.

Definition at line 9858 of file NPSMEFTd6.cpp.

9859 {
9860  double mu = 1.0;
9861 
9862  double dymu = deltaG_hff(leptons[MU]).real();
9863  double ymuSM = -(leptons[MU].getMass()) / v();
9864 
9865 // The ratio at all energies is given by a scaling of the muon Yukawa.
9866  mu = 1.0 + 2.0 * dymu/ymuSM ;
9867 
9868  if (FlagQuadraticTerms) {
9869  //Add contributions that are quadratic in the effective coefficients
9870  mu += dymu*dymu/ymuSM/ymuSM;
9871  }
9872 
9873  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
9874 
9875  return mu;
9876 }

◆ mupTVppWZ()

double NPSMEFTd6::mupTVppWZ ( const double  sqrt_s,
const double  pTV1,
const double  pTV2 
) const
virtual

The number of events in \( p p \to WZ\) in a given \(p_{TV}\) bin, normalized to the SM prediction. From arXiv: 1712.01310 [hep-ph] and private communication. Implemented only in NPSMEFTd6 class.

Returns
\(N_{ev}^{p_{TV}}/N_{ev,SM}^{p_{TV}}\)

Reimplemented from NPbase.

Definition at line 14611 of file NPSMEFTd6.cpp.

14612 {
14613  double mu = 1.0;
14614 
14615  double cHWp = 0.0;
14616 
14617  // In the Warsaw basis the contact interactions are generated only by CiHQ3 but
14618  // in the modified basis ODHW also contribute
14619  // Master Equations below are for cHWp = Ci/Lambda^2 in units of TeV^{-2},
14620  // but LambdaNP is in GeV. Add conversion factor.
14621 
14622  cHWp = 4.0 * (sW2_tree/eeMz2) * (CiHQ3_11 + (g2_tree/4.0) * CiDHW) * 1000000.0 / LambdaNP2;
14623 
14624 // Bin dependences assuming cutoff of the EFT at 5 TeV
14625 // Normalize to the total number of events to remove the dependence on Lumi
14626 // (Numbers correspond to 3/ab)
14627  if (sqrt_s == 14.0) {
14628 
14629  if (pTV1 == 100.){
14630  mu += (558.0 * cHWp + 56.8 * cHWp * cHWp) / 3450.0;
14631 
14632  } else if (pTV1 == 150.){
14633  mu += (410.0 * cHWp + 17.64 * cHWp * cHWp) / 2690.0;
14634 
14635  } else if (pTV1 == 220.){
14636  mu += (266.0 * cHWp + 45.6 * cHWp * cHWp) / 925.0;
14637 
14638  } else if (pTV1 == 300.){
14639  mu += (304.0 * cHWp + 108.0 * cHWp * cHWp) / 563.0;
14640 
14641  } else if (pTV1 == 500.){
14642  mu += (114.40 * cHWp + 96.8 * cHWp * cHWp) / 85.1 ;
14643 
14644  } else if (pTV1 == 750.){
14645  mu += (46.20 * cHWp + 86.8 * cHWp * cHWp) / 14.9;
14646 
14647  } else {
14648  throw std::runtime_error("Bad argument in NPSMEFTd6::mupTVppWZ()");
14649  }
14650 
14651  } else if (sqrt_s == 27.0) {
14652 
14653  if (pTV1 == 150.){
14654  mu += (824.0 * cHWp + 71.6 * cHWp * cHWp) / 5370.0;
14655 
14656  } else if (pTV1 == 220.){
14657  mu += (510.0 * cHWp + 75.2 * cHWp * cHWp) / 2210.0;
14658 
14659  } else if (pTV1 == 300.){
14660  mu += (808.0 * cHWp + 268.4 * cHWp * cHWp) / 1610.0;
14661 
14662  } else if (pTV1 == 500.){
14663  mu += (374.0 * cHWp + 308.0 * cHWp * cHWp) / 331.0;
14664 
14665  } else if (pTV1 == 750.){
14666  mu += (216.0 * cHWp + 420.0 * cHWp * cHWp) / 85.9;
14667 
14668  } else if (pTV1 == 1200.){
14669  mu += (78.2 * cHWp + 325.2 * cHWp * cHWp) / 10.0;
14670 
14671  } else {
14672  throw std::runtime_error("Bad argument in NPSMEFTd6::mupTVppWZ()");
14673  }
14674 
14675  } else if (sqrt_s == 100.0) {
14676 
14677  if (pTV1 == 220.){
14678  mu += (2000.0 * cHWp + 368.4 * cHWp * cHWp) / 8030.0;
14679 
14680  } else if (pTV1 == 300.){
14681  mu += (2780.0 * cHWp + 1000.0 * cHWp * cHWp) / 7270.0;
14682 
14683  } else if (pTV1 == 500.){
14684  mu += (1544.0 * cHWp + 1428.0 * cHWp * cHWp) / 2000.0;
14685 
14686  } else if (pTV1 == 750.){
14687  mu += (1256.0 * cHWp + 2668.0 * cHWp * cHWp) / 717.0;
14688 
14689  } else if (pTV1 == 1200.){
14690  mu += (678.0 * cHWp + 3400.0 * cHWp * cHWp) / 142.0;
14691 
14692  } else if (pTV1 == 1800.){
14693  mu += (234.0 * cHWp + 2540.0 * cHWp * cHWp) / 27.5;
14694 
14695  } else {
14696  throw std::runtime_error("Bad argument in NPSMEFTd6::mupTVppWZ()");
14697  }
14698 
14699  } else
14700  throw std::runtime_error("Bad argument in NPSMEFTd6::mupTVppWZ()");
14701 
14702  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
14703 
14704  return mu;
14705 
14706 }

◆ mutHq()

double NPSMEFTd6::mutHq ( const double  sqrt_s) const
virtual

The ratio \(\mu_{tHq}\) between the t-q-Higgs associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{tHq}\)

Reimplemented from NPbase.

Definition at line 8896 of file NPSMEFTd6.cpp.

8897 {
8898  double mu = 1.0;
8899 
8900  double C1 = 0.0;
8901 
8902  if (sqrt_s == 7.0) {
8903 
8904  C1 = 0.0;
8905 
8906  mu += 0.0;
8907 
8908  if (FlagQuadraticTerms) {
8909  //Add contributions that are quadratic in the effective coefficients
8910  mu += 0.0;
8911 
8912  }
8913 
8914  } else if (sqrt_s == 8.0) {
8915 
8916  C1 = 0.0;
8917 
8918  mu += 0.0;
8919 
8920  if (FlagQuadraticTerms) {
8921  //Add contributions that are quadratic in the effective coefficients
8922  mu += 0.0;
8923 
8924  }
8925 
8926  } else if (sqrt_s == 13.0) {
8927 
8928  C1 = 0.0;
8929 
8930  mu += 0.0;
8931 
8932  if (FlagQuadraticTerms) {
8933  //Add contributions that are quadratic in the effective coefficients
8934  mu += 0.0;
8935 
8936  }
8937 
8938  } else if (sqrt_s == 14.0) {
8939 
8940  C1 = 0.0;
8941 
8942  mu += 0.0;
8943 
8944  if (FlagQuadraticTerms) {
8945  //Add contributions that are quadratic in the effective coefficients
8946  mu += 0.0;
8947 
8948  }
8949 
8950  } else if (sqrt_s == 27.0) {
8951 
8952  C1 = 0.0;
8953 
8954  mu += 0.0;
8955 
8956  if (FlagQuadraticTerms) {
8957  //Add contributions that are quadratic in the effective coefficients
8958  mu += 0.0;
8959 
8960  }
8961 
8962  } else if (sqrt_s == 100.0) {
8963 
8964  C1 = 0.0;
8965 
8966  mu += 0.0;
8967 
8968  if (FlagQuadraticTerms) {
8969  //Add contributions that are quadratic in the effective coefficients
8970  mu += 0.0;
8971 
8972  }
8973 
8974  } else
8975  throw std::runtime_error("Bad argument in NPSMEFTd6::mutHq()");
8976 
8977  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
8978  //mu += etHqint + etHqpar;
8979 
8980 // Linear contribution from Higgs self-coupling
8981  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
8982 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
8984 
8985  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
8986 
8987  return mu;
8988 }

◆ muTHUggHbb()

double NPSMEFTd6::muTHUggHbb ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,bb}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,bb}\)

Reimplemented from NPbase.

Definition at line 13368 of file NPSMEFTd6.cpp.

13369 {
13370  if (FlagQuadraticTerms) {
13371  return ( muggH(sqrt_s)*BrHbbRatio() * (1.0 + eggFHbb ) * (1.0 + eHwidth)/(1.0 + eggFint + eggFpar)/(1.0 + eHbbint + eHbbpar) );
13372  } else {
13373  return ( muggH(sqrt_s) + BrHbbRatio() - 1.0 + eggFHbb - eggFint - eggFpar - eHbbint - eHbbpar + eHwidth );
13374  }
13375 }

◆ muTHUggHgaga()

double NPSMEFTd6::muTHUggHgaga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 12864 of file NPSMEFTd6.cpp.

12865 {
12866  if (FlagQuadraticTerms) {
12867  return ( muggH(sqrt_s)*BrHgagaRatio() * (1.0 + eggFHgaga ) * (1.0 + eHwidth)/(1.0 + eggFint + eggFpar)/(1.0 + eHgagaint + eHgagapar) );
12868  } else {
12869  return ( muggH(sqrt_s) + BrHgagaRatio() - 1.0 + eggFHgaga - eggFint - eggFpar - eHgagaint - eHgagapar + eHwidth );
12870  }
12871 }

◆ muTHUggHmumu()

double NPSMEFTd6::muTHUggHmumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,\mu\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,\mu\mu}\)

Reimplemented from NPbase.

Definition at line 13242 of file NPSMEFTd6.cpp.

13243 {
13244  if (FlagQuadraticTerms) {
13245  return ( muggH(sqrt_s)*BrHmumuRatio() * (1.0 + eggFHmumu ) * (1.0 + eHwidth)/(1.0 + eggFint + eggFpar)/(1.0 + eHmumuint + eHmumupar) );
13246  } else {
13247  return ( muggH(sqrt_s) + BrHmumuRatio() - 1.0 + eggFHmumu - eggFint - eggFpar - eHmumuint - eHmumupar + eHwidth );
13248  }
13249 }

◆ muTHUggHtautau()

double NPSMEFTd6::muTHUggHtautau ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,\tau\tau}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,\tau\tau}\)

Reimplemented from NPbase.

Definition at line 13305 of file NPSMEFTd6.cpp.

13306 {
13307  if (FlagQuadraticTerms) {
13308  return ( muggH(sqrt_s)*BrHtautauRatio() * (1.0 + eggFHtautau ) * (1.0 + eHwidth)/(1.0 + eggFint + eggFpar)/(1.0 + eHtautauint + eHtautaupar) );
13309  } else {
13310  return ( muggH(sqrt_s) + BrHtautauRatio() - 1.0 + eggFHtautau - eggFint - eggFpar - eHtautauint - eHtautaupar + eHwidth );
13311  }
13312 }

◆ muTHUggHWW()

double NPSMEFTd6::muTHUggHWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,WW}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,WW}\)

Reimplemented from NPbase.

Definition at line 13116 of file NPSMEFTd6.cpp.

13117 {
13118  if (FlagQuadraticTerms) {
13119  return ( muggH(sqrt_s)*BrHWWRatio() * (1.0 + eggFHWW ) * (1.0 + eHwidth)/(1.0 + eggFint + eggFpar)/(1.0 + eHWWint + eHWWpar) );
13120  } else {
13121  return ( muggH(sqrt_s) + BrHWWRatio() - 1.0 + eggFHWW - eggFint - eggFpar - eHWWint - eHWWpar + eHwidth );
13122  }
13123 }

◆ muTHUggHWW2l2v()

double NPSMEFTd6::muTHUggHWW2l2v ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,WW\to 2l2\nu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,WW\to 2l2\nu}\)

Reimplemented from NPbase.

Definition at line 13179 of file NPSMEFTd6.cpp.

13180 {
13181  if (FlagQuadraticTerms) {
13182  return ( muggH(sqrt_s)*BrHWW2l2vRatio() * (1.0 + eggFHWW ) * (1.0 + eHwidth)/(1.0 + eggFint + eggFpar)/(1.0 + eHWWint + eHWWpar) );
13183  } else {
13184  return ( muggH(sqrt_s) + BrHWW2l2vRatio() - 1.0 + eggFHWW - eggFint - eggFpar - eHWWint - eHWWpar + eHwidth );
13185  }
13186 }

◆ muTHUggHZga()

double NPSMEFTd6::muTHUggHZga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,Z\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,Z\gamma}\)

Reimplemented from NPbase.

Definition at line 12927 of file NPSMEFTd6.cpp.

12928 {
12929  if (FlagQuadraticTerms) {
12930  return ( muggH(sqrt_s)*BrHZgaRatio() * (1.0 + eggFHZga ) * (1.0 + eHwidth)/(1.0 + eggFint + eggFpar)/(1.0 + eHZgaint + eHZgapar) );
12931  } else {
12932  return ( muggH(sqrt_s) + BrHZgaRatio() - 1.0 + eggFHZga - eggFint - eggFpar - eHZgaint - eHZgapar + eHwidth );
12933  }
12934 }

◆ muTHUggHZgamumu()

double NPSMEFTd6::muTHUggHZgamumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,Z\gamma\to \gamma 2\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\to \gamma 2\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,Z\gamma\to \gamma 2\mu}\)

Reimplemented from NPbase.

Definition at line 13483 of file NPSMEFTd6.cpp.

13484 {
13485  if (FlagQuadraticTerms) {
13486  return ( muggH(sqrt_s)*BrHZgamumuRatio() * (1.0 + eggFHZga ) * (1.0 + eHwidth)/(1.0 + eggFint + eggFpar)/(1.0 + eHZgaint + eHZgapar) );
13487  } else {
13488  return ( muggH(sqrt_s) + BrHZgamumuRatio() - 1.0 + eggFHZga - eggFint - eggFpar - eHZgaint - eHZgapar + eHwidth );
13489  }
13490 }

◆ muTHUggHZZ()

double NPSMEFTd6::muTHUggHZZ ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,ZZ}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,ZZ}\)

Reimplemented from NPbase.

Definition at line 12990 of file NPSMEFTd6.cpp.

12991 {
12992  if (FlagQuadraticTerms) {
12993  return ( muggH(sqrt_s)*BrHZZRatio() * (1.0 + eggFHZZ ) * (1.0 + eHwidth)/(1.0 + eggFint + eggFpar)/(1.0 + eHZZint + eHZZpar) );
12994  } else {
12995  return ( muggH(sqrt_s) + BrHZZRatio() - 1.0 + eggFHZZ - eggFint - eggFpar - eHZZint - eHZZpar + eHwidth );
12996  }
12997 }

◆ muTHUggHZZ4l()

double NPSMEFTd6::muTHUggHZZ4l ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,ZZ\to 4l}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,ZZ\to 4l}\)

Reimplemented from NPbase.

Definition at line 13053 of file NPSMEFTd6.cpp.

13054 {
13055  if (FlagQuadraticTerms) {
13056  return ( muggH(sqrt_s)*BrHZZ4lRatio() * (1.0 + eggFHZZ ) * (1.0 + eHwidth)/(1.0 + eggFint + eggFpar)/(1.0 + eHZZint + eHZZpar) );
13057  } else {
13058  return ( muggH(sqrt_s) + BrHZZ4lRatio() - 1.0 + eggFHZZ - eggFint - eggFpar - eHZZint - eHZZpar + eHwidth );
13059  }
13060 }

◆ muTHUggHZZ4mu()

double NPSMEFTd6::muTHUggHZZ4mu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,ZZ\to 4\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,ZZ\to 4\mu}\)

Reimplemented from NPbase.

Definition at line 13474 of file NPSMEFTd6.cpp.

13475 {
13476  if (FlagQuadraticTerms) {
13477  return ( muggH(sqrt_s)*BrHZZ4muRatio() * (1.0 + eggFHZZ ) * (1.0 + eHwidth)/(1.0 + eggFint + eggFpar)/(1.0 + eHZZint + eHZZpar) );
13478  } else {
13479  return ( muggH(sqrt_s) + BrHZZ4muRatio() - 1.0 + eggFHZZ - eggFint - eggFpar - eHZZint - eHZZpar + eHwidth );
13480  }
13481 }

◆ muTHUttHbb()

double NPSMEFTd6::muTHUttHbb ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,bb}\) between the ttH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,bb}\)

Reimplemented from NPbase.

Definition at line 13422 of file NPSMEFTd6.cpp.

13423 {
13424  if (FlagQuadraticTerms) {
13425  return ( muttH(sqrt_s)*BrHbbRatio() * (1.0 + ettHbb ) * (1.0 + eHwidth)/(1.0 + eeettHint + eeettHpar)/(1.0 + eHbbint + eHbbpar) );
13426  } else {
13427  return ( muttH(sqrt_s) + BrHbbRatio() - 1.0 + ettHbb - eeettHint - eeettHpar - eHbbint - eHbbpar + eHwidth );
13428  }
13429 }

◆ muTHUttHgaga()

double NPSMEFTd6::muTHUttHgaga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,\gamma\gamma}\) between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 12918 of file NPSMEFTd6.cpp.

12919 {
12920  if (FlagQuadraticTerms) {
12921  return ( muttH(sqrt_s)*BrHgagaRatio() * (1.0 + ettHgaga ) * (1.0 + eHwidth)/(1.0 + eeettHint + eeettHpar)/(1.0 + eHgagaint + eHgagapar) );
12922  } else {
12923  return ( muttH(sqrt_s) + BrHgagaRatio() - 1.0 + ettHgaga - eeettHint - eeettHpar - eHgagaint - eHgagapar + eHwidth );
12924  }
12925 }

◆ muTHUttHmumu()

double NPSMEFTd6::muTHUttHmumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,\mu\mu}\) between the ttH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,\mu\mu}\)

Reimplemented from NPbase.

Definition at line 13296 of file NPSMEFTd6.cpp.

13297 {
13298  if (FlagQuadraticTerms) {
13299  return ( muttH(sqrt_s)*BrHmumuRatio() * (1.0 + ettHmumu ) * (1.0 + eHwidth)/(1.0 + eeettHint + eeettHpar)/(1.0 + eHmumuint + eHmumupar) );
13300  } else {
13301  return ( muttH(sqrt_s) + BrHmumuRatio() - 1.0 + ettHmumu - eeettHint - eeettHpar - eHmumuint - eHmumupar + eHwidth );
13302  }
13303 }

◆ muTHUttHtautau()

double NPSMEFTd6::muTHUttHtautau ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,\tau\tau}\) between the ttH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,\tau\tau}\)

Reimplemented from NPbase.

Definition at line 13359 of file NPSMEFTd6.cpp.

13360 {
13361  if (FlagQuadraticTerms) {
13362  return ( muttH(sqrt_s)*BrHtautauRatio() * (1.0 + ettHtautau ) * (1.0 + eHwidth)/(1.0 + eeettHint + eeettHpar)/(1.0 + eHtautauint + eHtautaupar) );
13363  } else {
13364  return ( muttH(sqrt_s) + BrHtautauRatio() - 1.0 + ettHtautau - eeettHint - eeettHpar - eHtautauint - eHtautaupar + eHwidth );
13365  }
13366 }

◆ muTHUttHWW()

double NPSMEFTd6::muTHUttHWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,WW}\) between the ttH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,WW}\)

Reimplemented from NPbase.

Definition at line 13170 of file NPSMEFTd6.cpp.

13171 {
13172  if (FlagQuadraticTerms) {
13173  return ( muttH(sqrt_s)*BrHWWRatio() * (1.0 + ettHWW ) * (1.0 + eHwidth)/(1.0 + eeettHint + eeettHpar)/(1.0 + eHWWint + eHWWpar) );
13174  } else {
13175  return ( muttH(sqrt_s) + BrHWWRatio() - 1.0 + ettHWW - eeettHint - eeettHpar - eHWWint - eHWWpar + eHwidth );
13176  }
13177 }

◆ muTHUttHWW2l2v()

double NPSMEFTd6::muTHUttHWW2l2v ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,WW\to 2l2\nu}\) between the ttH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,WW\to 2l2\nu}\)

Reimplemented from NPbase.

Definition at line 13233 of file NPSMEFTd6.cpp.

13234 {
13235  if (FlagQuadraticTerms) {
13236  return ( muttH(sqrt_s)*BrHWW2l2vRatio() * (1.0 + ettHWW ) * (1.0 + eHwidth)/(1.0 + eeettHint + eeettHpar)/(1.0 + eHWWint + eHWWpar) );
13237  } else {
13238  return ( muttH(sqrt_s) + BrHWW2l2vRatio() - 1.0 + ettHWW - eeettHint - eeettHpar - eHWWint - eHWWpar + eHwidth );
13239  }
13240 }

◆ muTHUttHZga()

double NPSMEFTd6::muTHUttHZga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,Z\gamma}\) between the ttH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,Z\gamma}\)

Reimplemented from NPbase.

Definition at line 12981 of file NPSMEFTd6.cpp.

12982 {
12983  if (FlagQuadraticTerms) {
12984  return ( muttH(sqrt_s)*BrHZgaRatio() * (1.0 + ettHZga ) * (1.0 + eHwidth)/(1.0 + eeettHint + eeettHpar)/(1.0 + eHZgaint + eHZgapar) );
12985  } else {
12986  return ( muttH(sqrt_s) + BrHZgaRatio() - 1.0 + ettHZga - eeettHint - eeettHpar - eHZgaint - eHZgapar + eHwidth );
12987  }
12988 }

◆ muTHUttHZZ()

double NPSMEFTd6::muTHUttHZZ ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,ZZ}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,ZZ}\)

Reimplemented from NPbase.

Definition at line 13044 of file NPSMEFTd6.cpp.

13045 {
13046  if (FlagQuadraticTerms) {
13047  return ( muttH(sqrt_s)*BrHZZRatio() * (1.0 + ettHZZ ) * (1.0 + eHwidth)/(1.0 + eeettHint + eeettHpar)/(1.0 + eHZZint + eHZZpar) );
13048  } else {
13049  return ( muttH(sqrt_s) + BrHZZRatio() - 1.0 + ettHZZ - eeettHint - eeettHpar - eHZZint - eHZZpar + eHwidth );
13050  }
13051 }

◆ muTHUttHZZ4l()

double NPSMEFTd6::muTHUttHZZ4l ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,ZZ\to 4l}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,ZZ\to 4l}\)

Reimplemented from NPbase.

Definition at line 13107 of file NPSMEFTd6.cpp.

13108 {
13109  if (FlagQuadraticTerms) {
13110  return ( muttH(sqrt_s)*BrHZZ4lRatio() * (1.0 + ettHZZ ) * (1.0 + eHwidth)/(1.0 + eeettHint + eeettHpar)/(1.0 + eHZZint + eHZZpar) );
13111  } else {
13112  return ( muttH(sqrt_s) + BrHZZ4lRatio() - 1.0 + ettHZZ - eeettHint - eeettHpar - eHZZint - eHZZpar + eHwidth );
13113  }
13114 }

◆ muTHUVBFBRinv()

double NPSMEFTd6::muTHUVBFBRinv ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF}\) between the VBF production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF}BR_{inv}\)

Reimplemented from NPbase.

Definition at line 13431 of file NPSMEFTd6.cpp.

13432 {
13433  return ( muVBF(sqrt_s)*Br_H_inv() * (1.0 + eVBFHinv )/(1.0 + eVBFint + eVBFpar) );
13434 }

◆ muTHUVBFHbb()

double NPSMEFTd6::muTHUVBFHbb ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,bb}\) between the VBF Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,bb}\)

Reimplemented from NPbase.

Definition at line 13377 of file NPSMEFTd6.cpp.

13378 {
13379  if (FlagQuadraticTerms) {
13380  return ( muVBF(sqrt_s)*BrHbbRatio() * (1.0 + eVBFHbb ) * (1.0 + eHwidth)/(1.0 + eVBFint + eVBFpar)/(1.0 + eHbbint + eHbbpar) );
13381  } else {
13382  return ( muVBF(sqrt_s) + BrHbbRatio() - 1.0 + eVBFHbb - eVBFint - eVBFpar - eHbbint - eHbbpar + eHwidth );
13383  }
13384 }

◆ muTHUVBFHgaga()

double NPSMEFTd6::muTHUVBFHgaga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,\gamma\gamma}\) between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 12873 of file NPSMEFTd6.cpp.

12874 {
12875  if (FlagQuadraticTerms) {
12876  return ( muVBF(sqrt_s)*BrHgagaRatio() * (1.0 + eVBFHgaga ) * (1.0 + eHwidth)/(1.0 + eVBFint + eVBFpar)/(1.0 + eHgagaint + eHgagapar) );
12877  } else {
12878  return ( muVBF(sqrt_s) + BrHgagaRatio() - 1.0 + eVBFHgaga - eVBFint - eVBFpar - eHgagaint - eHgagapar + eHwidth );
12879  }
12880 }

◆ muTHUVBFHinv()

double NPSMEFTd6::muTHUVBFHinv ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,inv}\) between the VBF production cross-section with subsequent decay into invisible states in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,inv}\)

Reimplemented from NPbase.

Definition at line 13436 of file NPSMEFTd6.cpp.

13437 {
13438  if (FlagQuadraticTerms) {
13439  return ( muVBF(sqrt_s)*BrHtoinvRatio() * (1.0 + eVBFHinv )/(1.0 + eVBFint + eVBFpar) );
13440  } else {
13441  return ( muVBF(sqrt_s) + BrHtoinvRatio() - 1.0 + eVBFHinv - eVBFint - eVBFpar );
13442  }
13443 }

◆ muTHUVBFHmumu()

double NPSMEFTd6::muTHUVBFHmumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,\mu\mu}\) between the VBF Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,\mu\mu}\)

Reimplemented from NPbase.

Definition at line 13251 of file NPSMEFTd6.cpp.

13252 {
13253  if (FlagQuadraticTerms) {
13254  return ( muVBF(sqrt_s)*BrHmumuRatio() * (1.0 + eVBFHmumu ) * (1.0 + eHwidth)/(1.0 + eVBFint + eVBFpar)/(1.0 + eHmumuint + eHmumupar) );
13255  } else {
13256  return ( muVBF(sqrt_s) + BrHmumuRatio() - 1.0 + eVBFHmumu - eVBFint - eVBFpar - eHmumuint - eHmumupar + eHwidth );
13257  }
13258 }

◆ muTHUVBFHtautau()

double NPSMEFTd6::muTHUVBFHtautau ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,\tau\tau}\) between the VBF Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,\tau\tau}\)

Reimplemented from NPbase.

Definition at line 13314 of file NPSMEFTd6.cpp.

13315 {
13316  if (FlagQuadraticTerms) {
13317  return ( muVBF(sqrt_s)*BrHtautauRatio() * (1.0 + eVBFHtautau ) * (1.0 + eHwidth)/(1.0 + eVBFint + eVBFpar)/(1.0 + eHtautauint + eHtautaupar) );
13318  } else {
13319  return ( muVBF(sqrt_s) + BrHtautauRatio() - 1.0 + eVBFHtautau - eVBFint - eVBFpar - eHtautauint - eHtautaupar + eHwidth );
13320  }
13321 }

◆ muTHUVBFHWW()

double NPSMEFTd6::muTHUVBFHWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,WW}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,WW}\)

Reimplemented from NPbase.

Definition at line 13125 of file NPSMEFTd6.cpp.

13126 {
13127  if (FlagQuadraticTerms) {
13128  return ( muVBF(sqrt_s)*BrHWWRatio() * (1.0 + eVBFHWW ) * (1.0 + eHwidth)/(1.0 + eVBFint + eVBFpar)/(1.0 + eHWWint + eHWWpar) );
13129  } else {
13130  return ( muVBF(sqrt_s) + BrHWWRatio() - 1.0 + eVBFHWW - eVBFint - eVBFpar - eHWWint - eHWWpar + eHwidth );
13131  }
13132 }

◆ muTHUVBFHWW2l2v()

double NPSMEFTd6::muTHUVBFHWW2l2v ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,WW\to 2l2\nu}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,WW\to 2l2\nu}\)

Reimplemented from NPbase.

Definition at line 13188 of file NPSMEFTd6.cpp.

13189 {
13190  if (FlagQuadraticTerms) {
13191  return ( muVBF(sqrt_s)*BrHWW2l2vRatio() * (1.0 + eVBFHWW ) * (1.0 + eHwidth)/(1.0 + eVBFint + eVBFpar)/(1.0 + eHWWint + eHWWpar) );
13192  } else {
13193  return ( muVBF(sqrt_s) + BrHWW2l2vRatio() - 1.0 + eVBFHWW - eVBFint - eVBFpar - eHWWint - eHWWpar + eHwidth );
13194  }
13195 }

◆ muTHUVBFHZga()

double NPSMEFTd6::muTHUVBFHZga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,Z\gamma}\) between the VBF Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,Z\gamma}\)

Reimplemented from NPbase.

Definition at line 12936 of file NPSMEFTd6.cpp.

12937 {
12938  if (FlagQuadraticTerms) {
12939  return ( muVBF(sqrt_s)*BrHZgaRatio() * (1.0 + eVBFHZga ) * (1.0 + eHwidth)/(1.0 + eVBFint + eVBFpar)/(1.0 + eHZgaint + eHZgapar) );
12940  } else {
12941  return ( muVBF(sqrt_s) + BrHZgaRatio() - 1.0 + eVBFHZga - eVBFint - eVBFpar - eHZgaint - eHZgapar + eHwidth );
12942  }
12943 }

◆ muTHUVBFHZZ()

double NPSMEFTd6::muTHUVBFHZZ ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,ZZ}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,ZZ}\)

Reimplemented from NPbase.

Definition at line 12999 of file NPSMEFTd6.cpp.

13000 {
13001  if (FlagQuadraticTerms) {
13002  return ( muVBF(sqrt_s)*BrHZZRatio() * (1.0 + eVBFHZZ ) * (1.0 + eHwidth)/(1.0 + eVBFint + eVBFpar)/(1.0 + eHZZint + eHZZpar) );
13003  } else {
13004  return ( muVBF(sqrt_s) + BrHZZRatio() - 1.0 + eVBFHZZ - eVBFint - eVBFpar - eHZZint - eHZZpar + eHwidth );
13005  }
13006 }

◆ muTHUVBFHZZ4l()

double NPSMEFTd6::muTHUVBFHZZ4l ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,ZZ\to 4l}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,ZZ\to 4l}\)

Reimplemented from NPbase.

Definition at line 13062 of file NPSMEFTd6.cpp.

13063 {
13064  if (FlagQuadraticTerms) {
13065  return ( muVBF(sqrt_s)*BrHZZ4lRatio() * (1.0 + eVBFHZZ ) * (1.0 + eHwidth)/(1.0 + eVBFint + eVBFpar)/(1.0 + eHZZint + eHZZpar) );
13066  } else {
13067  return ( muVBF(sqrt_s) + BrHZZ4lRatio() - 1.0 + eVBFHZZ - eVBFint - eVBFpar - eHZZint - eHZZpar + eHwidth );
13068  }
13069 }

◆ muTHUVHbb()

double NPSMEFTd6::muTHUVHbb ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,bb}\) between the VH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,bb}\)

Reimplemented from NPbase.

Definition at line 13404 of file NPSMEFTd6.cpp.

13405 {
13406  // Theory uncertainty in VH production, from the WH and ZH ones
13407  double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
13408  double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
13409  double eVHtot,eVHbb;
13410 
13411  eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13412 
13413  eVHbb = (eWHbb * sigmaWH_SM + eZHbb * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13414 
13415  if (FlagQuadraticTerms) {
13416  return ( muVH(sqrt_s)*BrHbbRatio() * (1.0 + eVHbb ) * (1.0 + eHwidth)/(1.0 + eVHtot)/(1.0 + eHbbint + eHbbpar) );
13417  } else {
13418  return ( muVH(sqrt_s) + BrHbbRatio() - 1.0 + eVHbb - eVHtot - eHbbint - eHbbpar + eHwidth );
13419  }
13420 }

◆ muTHUVHBRinv()

double NPSMEFTd6::muTHUVHBRinv ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH}\) between the VH production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH}BR_{inv}\)

Reimplemented from NPbase.

Definition at line 13445 of file NPSMEFTd6.cpp.

13446 {
13447  // Theory uncertainty in VH production, from the WH and ZH ones
13448  double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
13449  double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
13450  double eVHtot;
13451 
13452  eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13453 
13454  return ( muVH(sqrt_s)*Br_H_inv() * (1.0 + eVHinv )/(1.0 + eVHtot) );
13455 }

◆ muTHUVHgaga()

double NPSMEFTd6::muTHUVHgaga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,\gamma\gamma}\) between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 12900 of file NPSMEFTd6.cpp.

12901 {
12902  // Theory uncertainty in VH production, from the WH and ZH ones
12903  double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
12904  double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
12905  double eVHtot,eVHgaga;
12906 
12907  eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
12908 
12909  eVHgaga = (eWHgaga * sigmaWH_SM + eZHgaga * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
12910 
12911  if (FlagQuadraticTerms) {
12912  return ( muVH(sqrt_s)*BrHgagaRatio() * (1.0 + eVHgaga ) * (1.0 + eHwidth)/(1.0 + eVHtot)/(1.0 + eHgagaint + eHgagapar) );
12913  } else {
12914  return ( muVH(sqrt_s) + BrHgagaRatio() - 1.0 + eVHgaga - eVHtot - eHgagaint - eHgagapar + eHwidth );
12915  }
12916 }

◆ muTHUVHinv()

double NPSMEFTd6::muTHUVHinv ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,inv}\) between the VH production cross-section with subsequent decay into invisible states in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,inv}\)

Reimplemented from NPbase.

Definition at line 13457 of file NPSMEFTd6.cpp.

13458 {
13459  // Theory uncertainty in VH production, from the WH and ZH ones
13460  double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
13461  double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
13462  double eVHtot;
13463 
13464  eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13465 
13466  if (FlagQuadraticTerms) {
13467  return ( muVH(sqrt_s)*BrHtoinvRatio() * (1.0 + eVHinv )/(1.0 + eVHtot) );
13468  } else {
13469  return ( muVH(sqrt_s) + BrHtoinvRatio() - 1.0 + eVHinv - eVHtot );
13470  }
13471 }

◆ muTHUVHmumu()

double NPSMEFTd6::muTHUVHmumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,\mu\mu}\) between the VH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,\mu\mu}\)

Reimplemented from NPbase.

Definition at line 13278 of file NPSMEFTd6.cpp.

13279 {
13280  // Theory uncertainty in VH production, from the WH and ZH ones
13281  double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
13282  double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
13283  double eVHtot,eVHmumu;
13284 
13285  eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13286 
13287  eVHmumu = (eWHmumu * sigmaWH_SM + eZHmumu * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13288 
13289  if (FlagQuadraticTerms) {
13290  return ( muVH(sqrt_s)*BrHmumuRatio() * (1.0 + eVHmumu ) * (1.0 + eHwidth)/(1.0 + eVHtot)/(1.0 + eHmumuint + eHmumupar) );
13291  } else {
13292  return ( muVH(sqrt_s) + BrHmumuRatio() - 1.0 + eVHmumu - eVHtot - eHmumuint - eHmumupar + eHwidth );
13293  }
13294 }

◆ muTHUVHtautau()

double NPSMEFTd6::muTHUVHtautau ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,\tau\tau}\) between the VH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,\tau\tau}\)

Reimplemented from NPbase.

Definition at line 13341 of file NPSMEFTd6.cpp.

13342 {
13343  // Theory uncertainty in VH production, from the WH and ZH ones
13344  double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
13345  double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
13346  double eVHtot,eVHtautau;
13347 
13348  eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13349 
13350  eVHtautau = (eWHtautau * sigmaWH_SM + eZHtautau * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13351 
13352  if (FlagQuadraticTerms) {
13353  return ( muVH(sqrt_s)*BrHtautauRatio() * (1.0 + eVHtautau ) * (1.0 + eHwidth)/(1.0 + eVHtot)/(1.0 + eHtautauint + eHtautaupar) );
13354  } else {
13355  return ( muVH(sqrt_s) + BrHtautauRatio() - 1.0 + eVHtautau - eVHtot - eHtautauint - eHtautaupar + eHwidth );
13356  }
13357 }

◆ muTHUVHWW()

double NPSMEFTd6::muTHUVHWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,WW}\) between the VH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,WW}\)

Reimplemented from NPbase.

Definition at line 13152 of file NPSMEFTd6.cpp.

13153 {
13154  // Theory uncertainty in VH production, from the WH and ZH ones
13155  double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
13156  double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
13157  double eVHtot,eVHWW;
13158 
13159  eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13160 
13161  eVHWW = (eWHWW * sigmaWH_SM + eZHWW * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13162 
13163  if (FlagQuadraticTerms) {
13164  return ( muVH(sqrt_s)*BrHWWRatio() * (1.0 + eVHWW ) * (1.0 + eHwidth)/(1.0 + eVHtot)/(1.0 + eHWWint + eHWWpar) );
13165  } else {
13166  return ( muVH(sqrt_s) + BrHWWRatio() - 1.0 + eVHWW - eVHtot - eHWWint - eHWWpar + eHwidth );
13167  }
13168 }

◆ muTHUVHWW2l2v()

double NPSMEFTd6::muTHUVHWW2l2v ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,WW\to 2l2\nu}\) between the VH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,WW\to 2l2\nu}\)

Reimplemented from NPbase.

Definition at line 13215 of file NPSMEFTd6.cpp.

13216 {
13217  // Theory uncertainty in VH production, from the WH and ZH ones
13218  double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
13219  double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
13220  double eVHtot,eVHWW;
13221 
13222  eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13223 
13224  eVHWW = (eWHWW * sigmaWH_SM + eZHWW * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13225 
13226  if (FlagQuadraticTerms) {
13227  return ( muVH(sqrt_s)*BrHWW2l2vRatio() * (1.0 + eVHWW ) * (1.0 + eHwidth)/(1.0 + eVHtot)/(1.0 + eHWWint + eHWWpar) );
13228  } else {
13229  return ( muVH(sqrt_s) + BrHWW2l2vRatio() - 1.0 + eVHWW - eVHtot - eHWWint - eHWWpar + eHwidth );
13230  }
13231 }

◆ muTHUVHZga()

double NPSMEFTd6::muTHUVHZga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,Z\gamma}\) between the VH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,Z\gamma}\)

Reimplemented from NPbase.

Definition at line 12963 of file NPSMEFTd6.cpp.

12964 {
12965  // Theory uncertainty in VH production, from the WH and ZH ones
12966  double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
12967  double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
12968  double eVHtot,eVHZga;
12969 
12970  eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
12971 
12972  eVHZga = (eWHZga * sigmaWH_SM + eZHZga * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
12973 
12974  if (FlagQuadraticTerms) {
12975  return ( muVH(sqrt_s)*BrHZgaRatio() * (1.0 + eVHZga ) * (1.0 + eHwidth)/(1.0 + eVHtot)/(1.0 + eHZgaint + eHZgapar) );
12976  } else {
12977  return ( muVH(sqrt_s) + BrHZgaRatio() - 1.0 + eVHZga - eVHtot - eHZgaint - eHZgapar + eHwidth );
12978  }
12979 }

◆ muTHUVHZZ()

double NPSMEFTd6::muTHUVHZZ ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,ZZ}\) between the VH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,ZZ}\)

Reimplemented from NPbase.

Definition at line 13026 of file NPSMEFTd6.cpp.

13027 {
13028  // Theory uncertainty in VH production, from the WH and ZH ones
13029  double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
13030  double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
13031  double eVHtot,eVHZZ;
13032 
13033  eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13034 
13035  eVHZZ = (eWHZZ * sigmaWH_SM + eZHZZ * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13036 
13037  if (FlagQuadraticTerms) {
13038  return ( muVH(sqrt_s)*BrHZZRatio() * (1.0 + eVHZZ ) * (1.0 + eHwidth)/(1.0 + eVHtot)/(1.0 + eHZZint + eHZZpar) );
13039  } else {
13040  return ( muVH(sqrt_s) + BrHZZRatio() - 1.0 + eVHZZ - eVHtot - eHZZint - eHZZpar + eHwidth );
13041  }
13042 }

◆ muTHUVHZZ4l()

double NPSMEFTd6::muTHUVHZZ4l ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,ZZ\to 4l}\) between the VH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,ZZ\to 4l}\)

Reimplemented from NPbase.

Definition at line 13089 of file NPSMEFTd6.cpp.

13090 {
13091  // Theory uncertainty in VH production, from the WH and ZH ones
13092  double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
13093  double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
13094  double eVHtot,eVHZZ;
13095 
13096  eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13097 
13098  eVHZZ = (eWHZZ * sigmaWH_SM + eZHZZ * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13099 
13100  if (FlagQuadraticTerms) {
13101  return ( muVH(sqrt_s)*BrHZZ4lRatio() * (1.0 + eVHZZ ) * (1.0 + eHwidth)/(1.0 + eVHtot)/(1.0 + eHZZint + eHZZpar) );
13102  } else {
13103  return ( muVH(sqrt_s) + BrHZZ4lRatio() - 1.0 + eVHZZ - eVHtot - eHZZint - eHZZpar + eHwidth );
13104  }
13105 }

◆ muTHUWHbb()

double NPSMEFTd6::muTHUWHbb ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,bb}\) between the WH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,bb}\)

Reimplemented from NPbase.

Definition at line 13395 of file NPSMEFTd6.cpp.

13396 {
13397  if (FlagQuadraticTerms) {
13398  return ( muWH(sqrt_s)*BrHbbRatio() * (1.0 + eWHbb ) * (1.0 + eHwidth)/(1.0 + eWHint + eWHpar)/(1.0 + eHbbint + eHbbpar) );
13399  } else {
13400  return ( muWH(sqrt_s) + BrHbbRatio() - 1.0 + eWHbb - eWHint - eWHpar - eHbbint - eHbbpar + eHwidth );
13401  }
13402 }

◆ muTHUWHgaga()

double NPSMEFTd6::muTHUWHgaga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,\gamma\gamma}\) between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 12891 of file NPSMEFTd6.cpp.

12892 {
12893  if (FlagQuadraticTerms) {
12894  return ( muWH(sqrt_s)*BrHgagaRatio() * (1.0 + eWHgaga ) * (1.0 + eHwidth)/(1.0 + eWHint + eWHpar)/(1.0 + eHgagaint + eHgagapar) );
12895  } else {
12896  return ( muWH(sqrt_s) + BrHgagaRatio() - 1.0 + eWHgaga - eWHint - eWHpar - eHgagaint - eHgagapar + eHwidth );
12897  }
12898 }

◆ muTHUWHmumu()

double NPSMEFTd6::muTHUWHmumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,\mu\mu}\) between the WH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,\mu\mu}\)

Reimplemented from NPbase.

Definition at line 13269 of file NPSMEFTd6.cpp.

13270 {
13271  if (FlagQuadraticTerms) {
13272  return ( muWH(sqrt_s)*BrHmumuRatio() * (1.0 + eWHmumu ) * (1.0 + eHwidth)/(1.0 + eWHint + eWHpar)/(1.0 + eHmumuint + eHmumupar) );
13273  } else {
13274  return ( muWH(sqrt_s) + BrHmumuRatio() - 1.0 + eWHmumu - eWHint - eWHpar - eHmumuint - eHmumupar + eHwidth );
13275  }
13276 }

◆ muTHUWHtautau()

double NPSMEFTd6::muTHUWHtautau ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,\tau\tau}\) between the WH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,\tau\tau}\)

Reimplemented from NPbase.

Definition at line 13332 of file NPSMEFTd6.cpp.

13333 {
13334  if (FlagQuadraticTerms) {
13335  return ( muWH(sqrt_s)*BrHtautauRatio() * (1.0 + eWHtautau ) * (1.0 + eHwidth)/(1.0 + eWHint + eWHpar)/(1.0 + eHtautauint + eHtautaupar) );
13336  } else {
13337  return ( muWH(sqrt_s) + BrHtautauRatio() - 1.0 + eWHtautau - eWHint - eWHpar - eHtautauint - eHtautaupar + eHwidth );
13338  }
13339 }

◆ muTHUWHWW()

double NPSMEFTd6::muTHUWHWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,WW}\) between the WH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,WW}\)

Reimplemented from NPbase.

Definition at line 13143 of file NPSMEFTd6.cpp.

13144 {
13145  if (FlagQuadraticTerms) {
13146  return ( muWH(sqrt_s)*BrHWWRatio() * (1.0 + eWHWW ) * (1.0 + eHwidth)/(1.0 + eWHint + eWHpar)/(1.0 + eHWWint + eHWWpar) );
13147  } else {
13148  return ( muWH(sqrt_s) + BrHWWRatio() - 1.0 + eWHWW - eWHint - eWHpar - eHWWint - eHWWpar + eHwidth );
13149  }
13150 }

◆ muTHUWHWW2l2v()

double NPSMEFTd6::muTHUWHWW2l2v ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,WW\to 2l2\nu}\) between the WH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,WW\to 2l2\nu}\)

Reimplemented from NPbase.

Definition at line 13206 of file NPSMEFTd6.cpp.

13207 {
13208  if (FlagQuadraticTerms) {
13209  return ( muWH(sqrt_s)*BrHWW2l2vRatio() * (1.0 + eWHWW ) * (1.0 + eHwidth)/(1.0 + eWHint + eWHpar)/(1.0 + eHWWint + eHWWpar) );
13210  } else {
13211  return ( muWH(sqrt_s) + BrHWW2l2vRatio() - 1.0 + eWHWW - eWHint - eWHpar - eHWWint - eHWWpar + eHwidth );
13212  }
13213 }

◆ muTHUWHZga()

double NPSMEFTd6::muTHUWHZga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,Z\gamma}\) between the WH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,Z\gamma}\)

Reimplemented from NPbase.

Definition at line 12954 of file NPSMEFTd6.cpp.

12955 {
12956  if (FlagQuadraticTerms) {
12957  return ( muWH(sqrt_s)*BrHZgaRatio() * (1.0 + eWHZga ) * (1.0 + eHwidth)/(1.0 + eWHint + eWHpar)/(1.0 + eHZgaint + eHZgapar) );
12958  } else {
12959  return ( muWH(sqrt_s) + BrHZgaRatio() - 1.0 + eWHZga - eWHint - eWHpar - eHZgaint - eHZgapar + eHwidth );
12960  }
12961 }

◆ muTHUWHZZ()

double NPSMEFTd6::muTHUWHZZ ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,ZZ}\) between the WH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,ZZ}\)

Reimplemented from NPbase.

Definition at line 13017 of file NPSMEFTd6.cpp.

13018 {
13019  if (FlagQuadraticTerms) {
13020  return ( muWH(sqrt_s)*BrHZZRatio() * (1.0 + eWHZZ ) * (1.0 + eHwidth)/(1.0 + eWHint + eWHpar)/(1.0 + eHZZint + eHZZpar) );
13021  } else {
13022  return ( muWH(sqrt_s) + BrHZZRatio() - 1.0 + eWHZZ - eWHint - eWHpar - eHZZint - eHZZpar + eHwidth );
13023  }
13024 }

◆ muTHUWHZZ4l()

double NPSMEFTd6::muTHUWHZZ4l ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,ZZ\to 4l}\) between the WH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,ZZ\to 4l}\)

Reimplemented from NPbase.

Definition at line 13080 of file NPSMEFTd6.cpp.

13081 {
13082  if (FlagQuadraticTerms) {
13083  return ( muWH(sqrt_s)*BrHZZ4lRatio() * (1.0 + eWHZZ ) * (1.0 + eHwidth)/(1.0 + eWHint + eWHpar)/(1.0 + eHZZint + eHZZpar) );
13084  } else {
13085  return ( muWH(sqrt_s) + BrHZZ4lRatio() - 1.0 + eWHZZ - eWHint - eWHpar - eHZZint - eHZZpar + eHwidth );
13086  }
13087 }

◆ muTHUZHbb()

double NPSMEFTd6::muTHUZHbb ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,bb}\) between the ZH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,bb}\)

Reimplemented from NPbase.

Definition at line 13386 of file NPSMEFTd6.cpp.

13387 {
13388  if (FlagQuadraticTerms) {
13389  return ( muZH(sqrt_s)*BrHbbRatio() * (1.0 + eZHbb ) * (1.0 + eHwidth)/(1.0 + eZHint + eZHpar)/(1.0 + eHbbint + eHbbpar) );
13390  } else {
13391  return ( muZH(sqrt_s) + BrHbbRatio() - 1.0 + eZHbb - eZHint - eZHpar - eHbbint - eHbbpar + eHwidth );
13392  }
13393 }

◆ muTHUZHgaga()

double NPSMEFTd6::muTHUZHgaga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,\gamma\gamma}\) between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 12882 of file NPSMEFTd6.cpp.

12883 {
12884  if (FlagQuadraticTerms) {
12885  return ( muZH(sqrt_s)*BrHgagaRatio() * (1.0 + eZHgaga ) * (1.0 + eHwidth)/(1.0 + eZHint + eZHpar)/(1.0 + eHgagaint + eHgagapar) );
12886  } else {
12887  return ( muZH(sqrt_s) + BrHgagaRatio() - 1.0 + eZHgaga - eZHint - eZHpar - eHgagaint - eHgagapar + eHwidth );
12888  }
12889 }

◆ muTHUZHmumu()

double NPSMEFTd6::muTHUZHmumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,\mu\mu}\) between the ZH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,\mu\mu}\)

Reimplemented from NPbase.

Definition at line 13260 of file NPSMEFTd6.cpp.

13261 {
13262  if (FlagQuadraticTerms) {
13263  return ( muZH(sqrt_s)*BrHmumuRatio() * (1.0 + eZHmumu ) * (1.0 + eHwidth)/(1.0 + eZHint + eZHpar)/(1.0 + eHmumuint + eHmumupar) );
13264  } else {
13265  return ( muZH(sqrt_s) + BrHmumuRatio() - 1.0 + eZHmumu - eZHint - eZHpar - eHmumuint - eHmumupar + eHwidth );
13266  }
13267 }

◆ muTHUZHtautau()

double NPSMEFTd6::muTHUZHtautau ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,\tau\tau}\) between the ZH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,\tau\tau}\)

Reimplemented from NPbase.

Definition at line 13323 of file NPSMEFTd6.cpp.

13324 {
13325  if (FlagQuadraticTerms) {
13326  return ( muZH(sqrt_s)*BrHtautauRatio() * (1.0 + eZHtautau ) * (1.0 + eHwidth)/(1.0 + eZHint + eZHpar)/(1.0 + eHtautauint + eHtautaupar) );
13327  } else {
13328  return ( muZH(sqrt_s) + BrHtautauRatio() - 1.0 + eZHtautau - eZHint - eZHpar - eHtautauint - eHtautaupar + eHwidth );
13329  }
13330 }

◆ muTHUZHWW()

double NPSMEFTd6::muTHUZHWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,WW}\) between the ZH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,WW}\)

Reimplemented from NPbase.

Definition at line 13134 of file NPSMEFTd6.cpp.

13135 {
13136  if (FlagQuadraticTerms) {
13137  return ( muZH(sqrt_s)*BrHWWRatio() * (1.0 + eZHWW ) * (1.0 + eHwidth)/(1.0 + eZHint + eZHpar)/(1.0 + eHWWint + eHWWpar) );
13138  } else {
13139  return ( muZH(sqrt_s) + BrHWWRatio() - 1.0 + eZHWW - eZHint - eZHpar - eHWWint - eHWWpar + eHwidth );
13140  }
13141 }

◆ muTHUZHWW2l2v()

double NPSMEFTd6::muTHUZHWW2l2v ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,WW\to 2l2\nu}\) between the ZH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,WW\to 2l2\nu}\)

Reimplemented from NPbase.

Definition at line 13197 of file NPSMEFTd6.cpp.

13198 {
13199  if (FlagQuadraticTerms) {
13200  return ( muZH(sqrt_s)*BrHWW2l2vRatio() * (1.0 + eZHWW ) * (1.0 + eHwidth)/(1.0 + eZHint + eZHpar)/(1.0 + eHWWint + eHWWpar) );
13201  } else {
13202  return ( muZH(sqrt_s) + BrHWW2l2vRatio() - 1.0 + eZHWW - eZHint - eZHpar - eHWWint - eHWWpar + eHwidth );
13203  }
13204 }

◆ muTHUZHZga()

double NPSMEFTd6::muTHUZHZga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,Z\gamma}\) between the ZH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,Z\gamma}\)

Reimplemented from NPbase.

Definition at line 12945 of file NPSMEFTd6.cpp.

12946 {
12947  if (FlagQuadraticTerms) {
12948  return ( muZH(sqrt_s)*BrHZgaRatio() * (1.0 + eZHZga ) * (1.0 + eHwidth)/(1.0 + eZHint + eZHpar)/(1.0 + eHZgaint + eHZgapar) );
12949  } else {
12950  return ( muZH(sqrt_s) + BrHZgaRatio() - 1.0 + eZHZga - eZHint - eZHpar - eHZgaint - eHZgapar + eHwidth );
12951  }
12952 }

◆ muTHUZHZZ()

double NPSMEFTd6::muTHUZHZZ ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,ZZ}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,ZZ}\)

Reimplemented from NPbase.

Definition at line 13008 of file NPSMEFTd6.cpp.

13009 {
13010  if (FlagQuadraticTerms) {
13011  return ( muZH(sqrt_s)*BrHZZRatio() * (1.0 + eZHZZ ) * (1.0 + eHwidth)/(1.0 + eZHint + eZHpar)/(1.0 + eHZZint + eHZZpar) );
13012  } else {
13013  return ( muZH(sqrt_s) + BrHZZRatio() - 1.0 + eZHZZ - eZHint - eZHpar - eHZZint - eHZZpar + eHwidth );
13014  }
13015 }

◆ muTHUZHZZ4l()

double NPSMEFTd6::muTHUZHZZ4l ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,ZZ\to 4l}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,ZZ\to 4l}\)

Reimplemented from NPbase.

Definition at line 13071 of file NPSMEFTd6.cpp.

13072 {
13073  if (FlagQuadraticTerms) {
13074  return ( muZH(sqrt_s)*BrHZZ4lRatio() * (1.0 + eZHZZ ) * (1.0 + eHwidth)/(1.0 + eZHint + eZHpar)/(1.0 + eHZZint + eHZZpar) );
13075  } else {
13076  return ( muZH(sqrt_s) + BrHZZ4lRatio() - 1.0 + eZHZZ - eZHint - eZHpar - eHZZint - eHZZpar + eHwidth );
13077  }
13078 }

◆ muttH()

double NPSMEFTd6::muttH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH}\) between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH}\)

Reimplemented from NPbase.

Definition at line 8754 of file NPSMEFTd6.cpp.

8755 {
8756  double mu = 1.0;
8757 
8758  double C1 = 0.0;
8759 
8760  if (sqrt_s == 1.96) {
8761 
8762  C1 = 0.0; // N.A.
8763 
8764  mu +=
8765  +423420. * (1. + ettH_2_HG ) * CHG / LambdaNP2
8766  -4269.4 * (1. + ettH_2_G ) * CG / LambdaNP2
8767  +566792. * (1. + ettH_2_uG_33r ) * CiuG_33r / LambdaNP2
8768  -2.854 * (1. + ettH_2_DeltagHt ) * deltaG_hff(quarks[TOP]).real()
8769  ;
8770 
8771  if (FlagQuadraticTerms) {
8772  //Add contributions that are quadratic in the effective coefficients
8773  mu += 0.0;
8774 
8775  }
8776 
8777  } else if (sqrt_s == 7.0) {
8778 
8779  C1 = 0.0387;
8780 
8781  mu +=
8782  +532200. * (1. + ettH_78_HG ) * CHG / LambdaNP2
8783  -85145.2 * (1. + ettH_78_G ) * CG / LambdaNP2
8784  +811678. * (1. + ettH_78_uG_33r ) * CiuG_33r / LambdaNP2
8785  -2.841 * (1. + ettH_78_DeltagHt ) * deltaG_hff(quarks[TOP]).real()
8786  ;
8787 
8788  if (FlagQuadraticTerms) {
8789  //Add contributions that are quadratic in the effective coefficients
8790  mu += 0.0;
8791 
8792  }
8793 
8794  } else if (sqrt_s == 8.0) {
8795 
8796  C1 = 0.0378;
8797 
8798  mu +=
8799  +535632. * (1. + ettH_78_HG ) * CHG / LambdaNP2
8800  -86537.2 * (1. + ettH_78_G ) * CG / LambdaNP2
8801  +825379. * (1. + ettH_78_uG_33r ) * CiuG_33r / LambdaNP2
8802  -2.849 * (1. + ettH_78_DeltagHt ) * deltaG_hff(quarks[TOP]).real()
8803  ;
8804 
8805  if (FlagQuadraticTerms) {
8806  //Add contributions that are quadratic in the effective coefficients
8807  mu += 0.0;
8808 
8809  }
8810 
8811  } else if (sqrt_s == 13.0) {
8812 
8813  C1 = 0.0351;
8814 
8815  mu +=
8816  +538764. * (1. + ettH_1314_HG ) * CHG / LambdaNP2
8817  -84648. * (1. + ettH_1314_G ) * CG / LambdaNP2
8818  +860470. * (1. + ettH_1314_uG_33r ) * CiuG_33r / LambdaNP2
8819  -2.834 * (1. + ettH_1314_DeltagHt ) * deltaG_hff(quarks[TOP]).real()
8820  ;
8821 
8822  if (FlagQuadraticTerms) {
8823  //Add contributions that are quadratic in the effective coefficients
8824  mu += 0.0;
8825 
8826  }
8827 
8828  } else if (sqrt_s == 14.0) {
8829 
8830  C1 = 0.0347;
8831 
8832  mu +=
8833  +536600. * (1. + ettH_1314_HG ) * CHG / LambdaNP2
8834  -83824.6 * (1. + ettH_1314_G ) * CG / LambdaNP2
8835  +863670. * (1. + ettH_1314_uG_33r ) * CiuG_33r / LambdaNP2
8836  -2.839 * (1. + ettH_1314_DeltagHt ) * deltaG_hff(quarks[TOP]).real()
8837  ;
8838 
8839  if (FlagQuadraticTerms) {
8840  //Add contributions that are quadratic in the effective coefficients
8841  mu += 0.0;
8842 
8843  }
8844 
8845  } else if (sqrt_s == 27.0) {
8846 
8847  C1 = 0.0320; // From arXiv: 1902.00134
8848 
8849  mu +=
8850  +519682. * CHG / LambdaNP2
8851  -68463.1 * CG / LambdaNP2
8852  +884060. * CiuG_33r / LambdaNP2
8853  -2.849 * deltaG_hff(quarks[TOP]).real()
8854  ;
8855 
8856  if (FlagQuadraticTerms) {
8857  //Add contributions that are quadratic in the effective coefficients
8858  mu += 0.0;
8859 
8860  }
8861 
8862  } else if (sqrt_s == 100.0) {
8863 
8864  C1 = 0.0; // N.A.
8865 
8866  mu +=
8867  +467438. * CHG / LambdaNP2
8868  -22519. * CG / LambdaNP2
8869  +880378. * CiuG_33r / LambdaNP2
8870  -2.837 * deltaG_hff(quarks[TOP]).real()
8871  ;
8872 
8873  if (FlagQuadraticTerms) {
8874  //Add contributions that are quadratic in the effective coefficients
8875  mu += 0.0;
8876 
8877  }
8878 
8879  } else
8880  throw std::runtime_error("Bad argument in NPSMEFTd6::muttH()");
8881 
8882  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
8883  mu += ettHint + ettHpar;
8884 
8885 // Linear contribution from Higgs self-coupling
8886  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
8887 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
8889 
8890  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
8891 
8892  return mu;
8893 }

◆ muttHbb()

double NPSMEFTd6::muttHbb ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,bb}\) between the ttH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,bb}\)

Reimplemented from NPbase.

Definition at line 12852 of file NPSMEFTd6.cpp.

12853 {
12854  return muttH(sqrt_s) * BrHbbRatio();
12855 
12856 }

◆ muttHgaga()

double NPSMEFTd6::muttHgaga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,\gamma\gamma}\) between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 12564 of file NPSMEFTd6.cpp.

12565 {
12566  return muttH(sqrt_s) * BrHgagaRatio();
12567 
12568 }

◆ muttHmumu()

double NPSMEFTd6::muttHmumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,\mu\mu}\) between the ttH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,\mu\mu}\)

Reimplemented from NPbase.

Definition at line 12780 of file NPSMEFTd6.cpp.

12781 {
12782  return muttH(sqrt_s) * BrHmumuRatio();
12783 
12784 }

◆ muttHtautau()

double NPSMEFTd6::muttHtautau ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,\tau\tau}\) between the ttH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,\tau\tau}\)

Reimplemented from NPbase.

Definition at line 12816 of file NPSMEFTd6.cpp.

12817 {
12818  return muttH(sqrt_s) * BrHtautauRatio();
12819 
12820 }

◆ muttHWW()

double NPSMEFTd6::muttHWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,WW}\) between the ttH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,WW}\)

Reimplemented from NPbase.

Definition at line 12708 of file NPSMEFTd6.cpp.

12709 {
12710  return muttH(sqrt_s) * BrHWWRatio();
12711 
12712 }

◆ muttHWW2l2v()

double NPSMEFTd6::muttHWW2l2v ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,WW\to 2l2\nu}\) between the ttH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,WW\to 2l2\nu}\)

Reimplemented from NPbase.

Definition at line 12744 of file NPSMEFTd6.cpp.

12745 {
12746  return muttH(sqrt_s) * BrHWW2l2vRatio();
12747 
12748 }

◆ muttHZbbboost()

double NPSMEFTd6::muttHZbbboost ( const double  sqrt_s) const
virtual

The ratio \(\sigma(ttH)/\sigma(ttZ)\) in the \(H,Z\to b\bar{b}\) channel in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\sigma(ttH)/\sigma(ttZ)\) normalized to the SM

Reimplemented from NPbase.

Definition at line 12478 of file NPSMEFTd6.cpp.

12479 {
12480  /* Ratios of BR with the SM*/
12481  double BrHbbrat = BrHbbRatio();
12482  double BrZbbSM = (trueSM.GammaZ(quarks[BOTTOM]))/trueSM.Gamma_Z();
12483  double BrZbbrat = BR_Zf(quarks[BOTTOM])/BrZbbSM;
12484 
12485 // gslpp::complex dKappa_t = deltaG_hff(quarks[TOP]) / (-mtpole / v());
12486 // double dkt = dKappa_t.real();
12487 
12488 // double dgV = deltaGV_f(quarks[TOP]);
12489 // double dgA = deltaGA_f(quarks[TOP]);
12490 // double gLSM = quarks[TOP].getIsospin()
12491 // - (quarks[TOP].getCharge())*sW2_tree;
12492 // double gRSM = - (quarks[TOP].getCharge())*sW2_tree;
12493 
12494 // double dgL = 0.5*(dgV + dgA)/gLSM;
12495 // double dgR = 0.5*(dgV - dgA)/gRSM;
12496 
12497  double dsigmarat;
12498 
12499  /* VERY CRUDE APPROX. */
12500  //dsigmarat = 1.0 +
12501  // 2.0 * dkt -
12502  // 2.0 * (gLSM*gLSM*dgL + gRSM*gRSM*dgR)/(gLSM*gLSM + gRSM*gRSM);
12503 
12504  dsigmarat = 1.0;
12505 // ttH 100 TeV (from muttH func): NOT BOOSTED YET
12506  dsigmarat += +467438. * CHG / LambdaNP2
12507  -22519. * CG / LambdaNP2
12508  +880378. * CiuG_33r / LambdaNP2
12509  -2.837 * deltaG_hff(quarks[TOP]).real()
12510  ;
12511 // Divided (linearized) by ttZ 100 TeV
12512  dsigmarat = dsigmarat - (
12513  -40869.4 * CiHD / LambdaNP2
12514  -52607.9 * CiHWB / LambdaNP2
12515  -90424.9 * CHG / LambdaNP2
12516  +432089. * CG / LambdaNP2
12517  +326525. * CiuG_33r / LambdaNP2
12518  -2028.11 * CiuW_33r / LambdaNP2
12519  +1679.85 * CiuB_33r / LambdaNP2
12520  +1454.5 * CiHQ1_11 / LambdaNP2
12521  +1065.27 * CiHu_11 / LambdaNP2
12522  +82169.1 * CiHu_33 / LambdaNP2
12523  -1229.16 * CiHd_11 / LambdaNP2
12524  +6780.84 * CiHQ3_11 / LambdaNP2
12525  -1.374 * DeltaGF()
12526  +4.242 * -0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
12527  );
12528 
12529  return dsigmarat * (BrHbbrat / BrZbbrat);
12530 
12531 }

◆ muttHZga()

double NPSMEFTd6::muttHZga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,Z\gamma}\) between the ttH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,Z\gamma}\)

Reimplemented from NPbase.

Definition at line 12600 of file NPSMEFTd6.cpp.

12601 {
12602  return muttH(sqrt_s) * BrHZgaRatio();
12603 
12604 }

◆ muttHZZ()

double NPSMEFTd6::muttHZZ ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,ZZ}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,ZZ}\)

Reimplemented from NPbase.

Definition at line 12636 of file NPSMEFTd6.cpp.

12637 {
12638  return muttH(sqrt_s) * BrHZZRatio();
12639 
12640 }

◆ muttHZZ4l()

double NPSMEFTd6::muttHZZ4l ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,ZZ\to 4l}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,ZZ\to 4l}\)

Reimplemented from NPbase.

Definition at line 12672 of file NPSMEFTd6.cpp.

12673 {
12674  return muttH(sqrt_s) * BrHZZ4lRatio();
12675 
12676 }

◆ muVBF()

double NPSMEFTd6::muVBF ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF}\) between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF}\)

Reimplemented from NPbase.

Definition at line 3434 of file NPSMEFTd6.cpp.

3435 {
3436  double mu = 1.0;
3437 
3438  double C1 = 0.0;
3439 
3440  if (sqrt_s == 1.96) {
3441 
3442  C1 = 0.0; // N.A.
3443 
3444  mu +=
3445  +120936. * (1. + eVBF_2_Hbox ) * CiHbox / LambdaNP2
3446  -9422.68 * (1. + eVBF_2_HQ1_11 ) * CiHQ1_11 / LambdaNP2
3447  -10683.8 * (1. + eVBF_2_Hu_11 ) * CiHu_11 / LambdaNP2
3448  +4055.59 * (1. + eVBF_2_Hd_11 ) * CiHd_11 / LambdaNP2
3449  -229691. * (1. + eVBF_2_HQ3_11 ) * CiHQ3_11 / LambdaNP2
3450  -170093. * (1. + eVBF_2_HD ) * CiHD / LambdaNP2
3451  +8971.22 * (1. + eVBF_2_HB ) * CiHB / LambdaNP2
3452  -65827.6 * (1. + eVBF_2_HW ) * CiHW / LambdaNP2
3453  -323514. * (1. + eVBF_2_HWB ) * CiHWB / LambdaNP2
3454  +481332. * (1. + eVBF_2_HG ) * CHG / LambdaNP2
3455  +1255.16 * (1. + eVBF_2_DHB ) * CiDHB / LambdaNP2
3456  -34956.7 * (1. + eVBF_2_DHW ) * CiDHW / LambdaNP2
3457  -4.511 * (1. + eVBF_2_DeltaGF ) * DeltaGF()
3458  -3.481 * deltaMwd6()
3459  ;
3460 
3461  if (FlagQuadraticTerms) {
3462  //Add contributions that are quadratic in the effective coefficients
3463 
3464  mu += 0.0;
3465 
3466  }
3467 
3468  } else if (sqrt_s == 7.0) {
3469 
3470  C1 = 0.0065;
3471 
3472  mu +=
3473  +121582. * (1. + eVBF_78_Hbox ) * CiHbox / LambdaNP2
3474  +13546.6 * (1. + eVBF_78_HQ1_11 ) * CiHQ1_11 / LambdaNP2
3475  -27657.6 * (1. + eVBF_78_Hu_11 ) * CiHu_11 / LambdaNP2
3476  +8892.12 * (1. + eVBF_78_Hd_11 ) * CiHd_11 / LambdaNP2
3477  -411400. * (1. + eVBF_78_HQ3_11 ) * CiHQ3_11 / LambdaNP2
3478  -164286. * (1. + eVBF_78_HD ) * CiHD / LambdaNP2
3479  -423.123 * (1. + eVBF_78_HB ) * CiHB / LambdaNP2
3480  -89854. * (1. + eVBF_78_HW ) * CiHW / LambdaNP2
3481  -312617. * (1. + eVBF_78_HWB ) * CiHWB / LambdaNP2
3482  -82956.8 * (1. + eVBF_78_HG ) * CHG / LambdaNP2
3483  -279.08 * (1. + eVBF_78_DHB ) * CiDHB / LambdaNP2
3484  -54861. * (1. + eVBF_78_DHW ) * CiDHW / LambdaNP2
3485  -4.479 * (1. + eVBF_78_DeltaGF ) * DeltaGF()
3486  -3.22 * deltaMwd6()
3487  ;
3488 
3489  if (FlagQuadraticTerms) {
3490  //Add contributions that are quadratic in the effective coefficients
3491 
3492  mu += 0.0;
3493 
3494  }
3495 
3496  } else if (sqrt_s == 8.0) {
3497 
3498  C1 = 0.0065;
3499 
3500  mu +=
3501  +121042. * (1. + eVBF_78_Hbox ) * CiHbox / LambdaNP2
3502  +12739.3 * (1. + eVBF_78_HQ1_11 ) * CiHQ1_11 / LambdaNP2
3503  -28367.7 * (1. + eVBF_78_Hu_11 ) * CiHu_11 / LambdaNP2
3504  +9134.21 * (1. + eVBF_78_Hd_11 ) * CiHd_11 / LambdaNP2
3505  -423704. * (1. + eVBF_78_HQ3_11 ) * CiHQ3_11 / LambdaNP2
3506  -165182. * (1. + eVBF_78_HD ) * CiHD / LambdaNP2
3507  -349.242 * (1. + eVBF_78_HB ) * CiHB / LambdaNP2
3508  -87279.4 * (1. + eVBF_78_HW ) * CiHW / LambdaNP2
3509  -313449. * (1. + eVBF_78_HWB ) * CiHWB / LambdaNP2
3510  -69421.9 * (1. + eVBF_78_HG ) * CHG / LambdaNP2
3511  -373.338 * (1. + eVBF_78_DHB ) * CiDHB / LambdaNP2
3512  -57028.1 * (1. + eVBF_78_DHW ) * CiDHW / LambdaNP2
3513  -4.472 * (1. + eVBF_78_DeltaGF ) * DeltaGF()
3514  -3.138 * deltaMwd6()
3515  ;
3516 
3517  if (FlagQuadraticTerms) {
3518  //Add contributions that are quadratic in the effective coefficients
3519 
3520  mu += 0.0;
3521 
3522  }
3523  } else if (sqrt_s == 13.0) {
3524 
3525  C1 = 0.0064;
3526 
3527  mu +=
3528  +121798. * (1. + eVBF_1314_Hbox ) * CiHbox / LambdaNP2
3529  +10339.7 * (1. + eVBF_1314_HQ1_11 ) * CiHQ1_11 / LambdaNP2
3530  -30827.2 * (1. + eVBF_1314_Hu_11 ) * CiHu_11 / LambdaNP2
3531  +10564.3 * (1. + eVBF_1314_Hd_11 ) * CiHd_11 / LambdaNP2
3532  -466270. * (1. + eVBF_1314_HQ3_11 ) * CiHQ3_11 / LambdaNP2
3533  -164119. * (1. + eVBF_1314_HD ) * CiHD / LambdaNP2
3534  -61.471 * (1. + eVBF_1314_HB ) * CiHB / LambdaNP2
3535  -82985.3 * (1. + eVBF_1314_HW ) * CiHW / LambdaNP2
3536  -313815. * (1. + eVBF_1314_HWB ) * CiHWB / LambdaNP2
3537  -36554. * (1. + eVBF_1314_HG ) * CHG / LambdaNP2
3538  -725.694 * (1. + eVBF_1314_DHB ) * CiDHB / LambdaNP2
3539  -65253.4 * (1. + eVBF_1314_DHW ) * CiDHW / LambdaNP2
3540  -4.474 * (1. + eVBF_1314_DeltaGF ) * DeltaGF()
3541  -3.109 * deltaMwd6()
3542  ;
3543 
3544  if (FlagQuadraticTerms) {
3545  //Add contributions that are quadratic in the effective coefficients
3546  mu += 0.0;
3547  }
3548 
3549  } else if (sqrt_s == 14.0) {
3550 
3551  C1 = 0.0064;
3552 
3553  mu +=
3554  +120948. * (1. + eVBF_1314_Hbox ) * CiHbox / LambdaNP2
3555  +9896.36 * (1. + eVBF_1314_HQ1_11 ) * CiHQ1_11 / LambdaNP2
3556  -31371. * (1. + eVBF_1314_Hu_11 ) * CiHu_11 / LambdaNP2
3557  +10716.4 * (1. + eVBF_1314_Hd_11 ) * CiHd_11 / LambdaNP2
3558  -473497. * (1. + eVBF_1314_HQ3_11 ) * CiHQ3_11 / LambdaNP2
3559  -164672. * (1. + eVBF_1314_HD ) * CiHD / LambdaNP2
3560  -60.253 * (1. + eVBF_1314_HB ) * CiHB / LambdaNP2
3561  -83504.9 * (1. + eVBF_1314_HW ) * CiHW / LambdaNP2
3562  -314059. * (1. + eVBF_1314_HWB ) * CiHWB / LambdaNP2
3563  -33627.6 * (1. + eVBF_1314_HG ) * CHG / LambdaNP2
3564  -775.959 * (1. + eVBF_1314_DHB ) * CiDHB / LambdaNP2
3565  -66336.3 * (1. + eVBF_1314_DHW ) * CiDHW / LambdaNP2
3566  -4.474 * (1. + eVBF_1314_DeltaGF ) * DeltaGF()
3567  -3.193 * deltaMwd6()
3568  ;
3569 
3570  if (FlagQuadraticTerms) {
3571  //Add contributions that are quadratic in the effective coefficients
3572  mu += 0.0;
3573 
3574  }
3575 
3576  } else if (sqrt_s == 27.0) {
3577 
3578  C1 = 0.0062; // From arXiv: 1902.00134
3579 
3580  mu +=
3581  +120777. * CiHbox / LambdaNP2
3582  +6664.27 * CiHQ1_11 / LambdaNP2
3583  -34230.7 * CiHu_11 / LambdaNP2
3584  +12917.3 * CiHd_11 / LambdaNP2
3585  -536216. * CiHQ3_11 / LambdaNP2
3586  -163493. * CiHD / LambdaNP2
3587  +58.33 * CiHB / LambdaNP2
3588  -81360.5 * CiHW / LambdaNP2
3589  -313026. * CiHWB / LambdaNP2
3590  -16430. * CHG / LambdaNP2
3591  -1314.45 * CiDHB / LambdaNP2
3592  -75884.6 * CiDHW / LambdaNP2
3593  -4.475 * DeltaGF()
3594  -2.99 * deltaMwd6()
3595  ;
3596 
3597  if (FlagQuadraticTerms) {
3598  //Add contributions that are quadratic in the effective coefficients
3599  mu += 0.0;
3600 
3601  }
3602 
3603  } else if (sqrt_s == 100.0) {
3604 
3605  C1 = 0.0; // N.A.
3606 
3607  mu +=
3608  +121714. * CiHbox / LambdaNP2
3609  -2261.73 * CiHQ1_11 / LambdaNP2
3610  -42045.4 * CiHu_11 / LambdaNP2
3611  +17539.2 * CiHd_11 / LambdaNP2
3612  -674206. * CiHQ3_11 / LambdaNP2
3613  -163344. * CiHD / LambdaNP2
3614  +71.488 * CiHB / LambdaNP2
3615  -90808.2 * CiHW / LambdaNP2
3616  -312544. * CiHWB / LambdaNP2
3617  -8165.65 * CHG / LambdaNP2
3618  -2615.48 * CiDHB / LambdaNP2
3619  -96539.6 * CiDHW / LambdaNP2
3620  -4.452 * DeltaGF()
3621  -2.949 * deltaMwd6()
3622  ;
3623 
3624  if (FlagQuadraticTerms) {
3625  //Add contributions that are quadratic in the effective coefficients
3626  mu += 0.0;
3627 
3628  }
3629 
3630  } else
3631  throw std::runtime_error("Bad argument in NPSMEFTd6::muVBF()");
3632 
3633  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
3634  mu += eVBFint + eVBFpar;
3635 
3636 // Linear contribution from Higgs self-coupling
3637  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
3638 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
3640 
3641  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
3642 
3643  return mu;
3644 }

◆ muVBFgamma()

double NPSMEFTd6::muVBFgamma ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF+\gamma}\) between the vector-boson fusion Higgs production cross-section in association with a hard photon in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF+\gamma}\)

Reimplemented from NPbase.

Definition at line 3649 of file NPSMEFTd6.cpp.

3650 {
3651  double mu = 1.0;
3652 
3653  double C1 = 0.0; //Use same values as VBF
3654 
3655  if (sqrt_s == 13.0) {
3656 
3657  C1 = 0.0064;
3658 
3659  mu +=
3660  +119630. * CiHbox / LambdaNP2
3661  -501300. * CiHQ3_11 / LambdaNP2
3662  -200890. * CiHD / LambdaNP2
3663  +11852.5 * CiHB / LambdaNP2
3664  -131586. * CiHW / LambdaNP2
3665  -361991. * CiHWB / LambdaNP2
3666  -18894.5 * CiDHB / LambdaNP2
3667  -69025.4 * CiDHW / LambdaNP2
3668  +23773.1 * CiW / LambdaNP2
3669  -4.629 * DeltaGF()
3670  -5.637 * deltaMwd6()
3671  ;
3672 
3673  if (FlagQuadraticTerms) {
3674  //Add contributions that are quadratic in the effective coefficients
3675  mu += 0.0;
3676  }
3677 
3678  } else
3679  throw std::runtime_error("Bad argument in NPSMEFTd6::muVBFgamma()");
3680 
3681  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy. Use same as VBF.)
3682  mu += eVBFint + eVBFpar;
3683 
3684 // Linear contribution from Higgs self-coupling
3685  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
3686 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
3688 
3689  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
3690 
3691  return mu;
3692 }

◆ muVBFHbb()

double NPSMEFTd6::muVBFHbb ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,bb}\) between the VBF Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,bb}\)

Reimplemented from NPbase.

Definition at line 12828 of file NPSMEFTd6.cpp.

12829 {
12830  return muVBF(sqrt_s) * BrHbbRatio();
12831 
12832 }

◆ muVBFHgaga()

double NPSMEFTd6::muVBFHgaga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,\gamma\gamma}\) between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 12540 of file NPSMEFTd6.cpp.

12541 {
12542  return muVBF(sqrt_s) * BrHgagaRatio();
12543 
12544 }

◆ muVBFHmumu()

double NPSMEFTd6::muVBFHmumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,\mu\mu}\) between the VBF Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,\mu\mu}\)

Reimplemented from NPbase.

Definition at line 12756 of file NPSMEFTd6.cpp.

12757 {
12758  return muVBF(sqrt_s) * BrHmumuRatio();
12759 
12760 }

◆ muVBFHtautau()

double NPSMEFTd6::muVBFHtautau ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,\tau\tau}\) between the VBF Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,\tau\tau}\)

Reimplemented from NPbase.

Definition at line 12792 of file NPSMEFTd6.cpp.

12793 {
12794  return muVBF(sqrt_s) * BrHtautauRatio();
12795 
12796 }

◆ muVBFHWW()

double NPSMEFTd6::muVBFHWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,WW}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,WW}\)

Reimplemented from NPbase.

Definition at line 12684 of file NPSMEFTd6.cpp.

12685 {
12686  return muVBF(sqrt_s) * BrHWWRatio();
12687 
12688 }

◆ muVBFHWW2l2v()

double NPSMEFTd6::muVBFHWW2l2v ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,WW\to 2l2\nu}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,WW\to 2l2\nu}\)

Reimplemented from NPbase.

Definition at line 12720 of file NPSMEFTd6.cpp.

12721 {
12722  return muVBF(sqrt_s) * BrHWW2l2vRatio();
12723 
12724 }

◆ muVBFHZga()

double NPSMEFTd6::muVBFHZga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,Z\gamma}\) between the VBF Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,Z\gamma}\)

Reimplemented from NPbase.

Definition at line 12576 of file NPSMEFTd6.cpp.

12577 {
12578  return muVBF(sqrt_s) * BrHZgaRatio();
12579 
12580 }

◆ muVBFHZZ()

double NPSMEFTd6::muVBFHZZ ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,ZZ}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,ZZ}\)

Reimplemented from NPbase.

Definition at line 12612 of file NPSMEFTd6.cpp.

12613 {
12614  return muVBF(sqrt_s) * BrHZZRatio();
12615 
12616 }

◆ muVBFHZZ4l()

double NPSMEFTd6::muVBFHZZ4l ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,ZZ\to 4l}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,ZZ\to 4l}\)

Reimplemented from NPbase.

Definition at line 12648 of file NPSMEFTd6.cpp.

12649 {
12650  return muVBF(sqrt_s) * BrHZZ4lRatio();
12651 
12652 }

◆ muVBFpVH()

double NPSMEFTd6::muVBFpVH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF+VH}\) between the sum of VBF and WH+ZH associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF+VH}\)

Reimplemented from NPbase.

Definition at line 8739 of file NPSMEFTd6.cpp.

8740 {
8741  double sigmaWH_SM = computeSigmaWH(sqrt_s);
8742  double sigmaZH_SM = computeSigmaZH(sqrt_s);
8743  double sigmaVBF_SM = computeSigmaVBF(sqrt_s);
8744  double sigmaWH = muWH(sqrt_s) * sigmaWH_SM;
8745  double sigmaZH = muZH(sqrt_s) * sigmaZH_SM;
8746  double sigmaVBF = muVBF(sqrt_s) * sigmaVBF_SM;
8747  double mu = ((sigmaWH + sigmaZH + sigmaVBF) / (sigmaWH_SM + sigmaZH_SM + sigmaVBF_SM));
8748 
8749  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
8750 
8751  return mu;
8752 }

◆ muVH()

double NPSMEFTd6::muVH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH}\) between the WH+ZH associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH}\)

Reimplemented from NPbase.

Definition at line 8726 of file NPSMEFTd6.cpp.

8727 {
8728  double sigmaWH_SM = computeSigmaWH(sqrt_s);
8729  double sigmaZH_SM = computeSigmaZH(sqrt_s);
8730  double sigmaWH = muWH(sqrt_s) * sigmaWH_SM;
8731  double sigmaZH = muZH(sqrt_s) * sigmaZH_SM;
8732  double mu = ((sigmaWH + sigmaZH) / (sigmaWH_SM + sigmaZH_SM));
8733 
8734  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
8735 
8736  return mu;
8737 }

◆ muVHbb()

double NPSMEFTd6::muVHbb ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,bb}\) between the VH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,bb}\)

Reimplemented from NPbase.

Definition at line 12846 of file NPSMEFTd6.cpp.

12847 {
12848  return muVH(sqrt_s) * BrHbbRatio();
12849 
12850 }

◆ muVHgaga()

double NPSMEFTd6::muVHgaga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,\gamma\gamma}\) between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 12558 of file NPSMEFTd6.cpp.

12559 {
12560  return muVH(sqrt_s) * BrHgagaRatio();
12561 
12562 }

◆ muVHmumu()

double NPSMEFTd6::muVHmumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,\mu\mu}\) between the VH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,\mu\mu}\)

Reimplemented from NPbase.

Definition at line 12774 of file NPSMEFTd6.cpp.

12775 {
12776  return muVH(sqrt_s) * BrHmumuRatio();
12777 
12778 }

◆ muVHtautau()

double NPSMEFTd6::muVHtautau ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,\tau\tau}\) between the VH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,\tau\tau}\)

Reimplemented from NPbase.

Definition at line 12810 of file NPSMEFTd6.cpp.

12811 {
12812  return muVH(sqrt_s) * BrHtautauRatio();
12813 
12814 }

◆ muVHWW()

double NPSMEFTd6::muVHWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,WW}\) between the VH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,WW}\)

Reimplemented from NPbase.

Definition at line 12702 of file NPSMEFTd6.cpp.

12703 {
12704  return muVH(sqrt_s) * BrHWWRatio();
12705 
12706 }

◆ muVHWW2l2v()

double NPSMEFTd6::muVHWW2l2v ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,WW\to 2l2\nu}\) between the VH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,WW\to 2l2\nu}\)

Reimplemented from NPbase.

Definition at line 12738 of file NPSMEFTd6.cpp.

12739 {
12740  return muVH(sqrt_s) * BrHWW2l2vRatio();
12741 
12742 }

◆ muVHZga()

double NPSMEFTd6::muVHZga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,Z\gamma}\) between the VH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,Z\gamma}\)

Reimplemented from NPbase.

Definition at line 12594 of file NPSMEFTd6.cpp.

12595 {
12596  return muVH(sqrt_s) * BrHZgaRatio();
12597 
12598 }

◆ muVHZZ()

double NPSMEFTd6::muVHZZ ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,ZZ}\) between the VH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,ZZ}\)

Reimplemented from NPbase.

Definition at line 12630 of file NPSMEFTd6.cpp.

12631 {
12632  return muVH(sqrt_s) * BrHZZRatio();
12633 
12634 }

◆ muVHZZ4l()

double NPSMEFTd6::muVHZZ4l ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,ZZ\to 4l}\) between the VH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,ZZ\to 4l}\)

Reimplemented from NPbase.

Definition at line 12666 of file NPSMEFTd6.cpp.

12667 {
12668  return muVH(sqrt_s) * BrHZZ4lRatio();
12669 
12670 }

◆ muWH()

double NPSMEFTd6::muWH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH}\)

Reimplemented from NPbase.

Definition at line 6864 of file NPSMEFTd6.cpp.

6865 {
6866  double mu = 1.0;
6867 
6868  double C1 = 0.0;
6869 
6870  if (sqrt_s == 1.96) {
6871 
6872  C1 = 0.0; // N.A.
6873 
6874  mu +=
6875  +121173. * (1. + eWH_2_Hbox ) * CiHbox / LambdaNP2
6876  +1566788. * (1. + eWH_2_HQ3_11 ) * CiHQ3_11 / LambdaNP2
6877  -160914. * (1. + eWH_2_HD ) * CiHD / LambdaNP2
6878  +860916. * (1. + eWH_2_HW ) * CiHW / LambdaNP2
6879  -286409. * (1. + eWH_2_HWB ) * CiHWB / LambdaNP2
6880  +134641. * (1. + eWH_2_DHW ) * CiDHW / LambdaNP2
6881  -3.31 * (1. + eWH_2_DeltaGF ) * DeltaGF()
6882  -2.199 * deltaMwd6()
6883  ;
6884 
6885  if (FlagQuadraticTerms) {
6886  //Add contributions that are quadratic in the effective coefficients
6887  mu += 0.0;
6888 
6889  }
6890 
6891  } else if (sqrt_s == 7.0) {
6892 
6893  C1 = 0.0106;
6894 
6895  mu +=
6896  +121015. * (1. + eWH_78_Hbox ) * CiHbox / LambdaNP2
6897  +1792020. * (1. + eWH_78_HQ3_11 ) * CiHQ3_11 / LambdaNP2
6898  -159689. * (1. + eWH_78_HD ) * CiHD / LambdaNP2
6899  +881065. * (1. + eWH_78_HW ) * CiHW / LambdaNP2
6900  -283895. * (1. + eWH_78_HWB ) * CiHWB / LambdaNP2
6901  +168173. * (1. + eWH_78_DHW ) * CiDHW / LambdaNP2
6902  -3.273 * (1. + eWH_78_DeltaGF ) * DeltaGF()
6903  -2.143 * deltaMwd6()
6904  ;
6905 
6906  if (FlagQuadraticTerms) {
6907  //Add contributions that are quadratic in the effective coefficients
6908  mu += 0.0;
6909 
6910  }
6911 
6912  } else if (sqrt_s == 8.0) {
6913 
6914  C1 = 0.0105;
6915 
6916  mu +=
6917  +121226. * (1. + eWH_78_Hbox ) * CiHbox / LambdaNP2
6918  +1830192. * (1. + eWH_78_HQ3_11 ) * CiHQ3_11 / LambdaNP2
6919  -159543. * (1. + eWH_78_HD ) * CiHD / LambdaNP2
6920  +884671. * (1. + eWH_78_HW ) * CiHW / LambdaNP2
6921  -283662. * (1. + eWH_78_HWB ) * CiHWB / LambdaNP2
6922  +174061. * (1. + eWH_78_DHW ) * CiDHW / LambdaNP2
6923  -3.278 * (1. + eWH_78_DeltaGF ) * DeltaGF()
6924  -2.147 * deltaMwd6()
6925  ;
6926 
6927  if (FlagQuadraticTerms) {
6928  //Add contributions that are quadratic in the effective coefficients
6929  mu += 0.0;
6930 
6931  }
6932 
6933  } else if (sqrt_s == 13.0) {
6934 
6935  C1 = 0.0103;
6936 
6937  mu +=
6938  +120439. * (1. + eWH_1314_Hbox ) * CiHbox / LambdaNP2
6939  +1953200. * (1. + eWH_1314_HQ3_11 ) * CiHQ3_11 / LambdaNP2
6940  -159847. * (1. + eWH_1314_HD ) * CiHD / LambdaNP2
6941  +892264. * (1. + eWH_1314_HW ) * CiHW / LambdaNP2
6942  -283830. * (1. + eWH_1314_HWB ) * CiHWB / LambdaNP2
6943  +192168. * (1. + eWH_1314_DHW ) * CiDHW / LambdaNP2
6944  -3.269 * (1. + eWH_1314_DeltaGF ) * DeltaGF()
6945  -2.101 * deltaMwd6()
6946  ;
6947 
6948  if (FlagQuadraticTerms) {
6949  //Add contributions that are quadratic in the effective coefficients
6950  mu += 0.0;
6951 
6952  }
6953 
6954  } else if (sqrt_s == 14.0) {
6955 
6956  C1 = 0.0103;
6957 
6958  mu +=
6959  +120284. * (1. + eWH_1314_Hbox ) * CiHbox / LambdaNP2
6960  +1971011. * (1. + eWH_1314_HQ3_11 ) * CiHQ3_11 / LambdaNP2
6961  -159830. * (1. + eWH_1314_HD ) * CiHD / LambdaNP2
6962  +893216. * (1. + eWH_1314_HW ) * CiHW / LambdaNP2
6963  -283818. * (1. + eWH_1314_HWB ) * CiHWB / LambdaNP2
6964  +194877. * (1. + eWH_1314_DHW ) * CiDHW / LambdaNP2
6965  -3.272 * (1. + eWH_1314_DeltaGF ) * DeltaGF()
6966  -2.103 * deltaMwd6()
6967  ;
6968 
6969  if (FlagQuadraticTerms) {
6970  //Add contributions that are quadratic in the effective coefficients
6971  mu += 0.0;
6972 
6973  }
6974 
6975  } else if (sqrt_s == 27.0) {
6976 
6977  C1 = 0.0101; // From arXiv: 1902.00134
6978 
6979  mu +=
6980  +120696. * CiHbox / LambdaNP2
6981  +2105646. * CiHQ3_11 / LambdaNP2
6982  -159695. * CiHD / LambdaNP2
6983  +900162. * CiHW / LambdaNP2
6984  -283257. * CiHWB / LambdaNP2
6985  +215592. * CiDHW / LambdaNP2
6986  -3.256 * DeltaGF()
6987  -2.063 * deltaMwd6()
6988  ;
6989 
6990  if (FlagQuadraticTerms) {
6991  //Add contributions that are quadratic in the effective coefficients
6992  mu += 0.0;
6993 
6994  }
6995 
6996  } else if (sqrt_s == 100.0) {
6997 
6998  C1 = 0.0; // N.A.
6999 
7000  mu +=
7001  +121319. * CiHbox / LambdaNP2
7002  +2294991. * CiHQ3_11 / LambdaNP2
7003  -159242. * CiHD / LambdaNP2
7004  +908130. * CiHW / LambdaNP2
7005  -282574. * CiHWB / LambdaNP2
7006  +245406. * CiDHW / LambdaNP2
7007  -3.259 * DeltaGF()
7008  -2.047 * deltaMwd6()
7009  ;
7010 
7011  if (FlagQuadraticTerms) {
7012  //Add contributions that are quadratic in the effective coefficients
7013  mu += 0.0;
7014 
7015  }
7016 
7017  } else
7018  throw std::runtime_error("Bad argument in NPSMEFTd6::muWH()");
7019 
7020  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
7021  mu += eWHint + eWHpar;
7022 
7023 // Linear contribution from Higgs self-coupling
7024  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
7025 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
7027 
7028  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
7029 
7030  return mu;
7031 }

◆ muWHbb()

double NPSMEFTd6::muWHbb ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,bb}\) between the WH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,bb}\)

Reimplemented from NPbase.

Definition at line 12840 of file NPSMEFTd6.cpp.

12841 {
12842  return muWH(sqrt_s) * BrHbbRatio();
12843 
12844 }

◆ muWHgaga()

double NPSMEFTd6::muWHgaga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,\gamma\gamma}\) between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 12552 of file NPSMEFTd6.cpp.

12553 {
12554  return muWH(sqrt_s) * BrHgagaRatio();
12555 
12556 }

◆ muWHmumu()

double NPSMEFTd6::muWHmumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,\mu\mu}\) between the WH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,\mu\mu}\)

Reimplemented from NPbase.

Definition at line 12768 of file NPSMEFTd6.cpp.

12769 {
12770  return muWH(sqrt_s) * BrHmumuRatio();
12771 
12772 }

◆ muWHtautau()

double NPSMEFTd6::muWHtautau ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,\tau\tau}\) between the WH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,\tau\tau}\)

Reimplemented from NPbase.

Definition at line 12804 of file NPSMEFTd6.cpp.

12805 {
12806  return muWH(sqrt_s) * BrHtautauRatio();
12807 
12808 }

◆ muWHWW()

double NPSMEFTd6::muWHWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,WW}\) between the WH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,WW}\)

Reimplemented from NPbase.

Definition at line 12696 of file NPSMEFTd6.cpp.

12697 {
12698  return muWH(sqrt_s) * BrHWWRatio();
12699 
12700 }

◆ muWHWW2l2v()

double NPSMEFTd6::muWHWW2l2v ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,WW\to 2l2\nu}\) between the WH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,WW\to 2l2\nu}\)

Reimplemented from NPbase.

Definition at line 12732 of file NPSMEFTd6.cpp.

12733 {
12734  return muWH(sqrt_s) * BrHWW2l2vRatio();
12735 
12736 }

◆ muWHZga()

double NPSMEFTd6::muWHZga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,Z\gamma}\) between the WH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,Z\gamma}\)

Reimplemented from NPbase.

Definition at line 12588 of file NPSMEFTd6.cpp.

12589 {
12590  return muWH(sqrt_s) * BrHZgaRatio();
12591 
12592 }

◆ muWHZZ()

double NPSMEFTd6::muWHZZ ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,ZZ}\) between the WH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,ZZ}\)

Reimplemented from NPbase.

Definition at line 12624 of file NPSMEFTd6.cpp.

12625 {
12626  return muWH(sqrt_s) * BrHZZRatio();
12627 
12628 }

◆ muWHZZ4l()

double NPSMEFTd6::muWHZZ4l ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,ZZ\to 4l}\) between the WH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,ZZ\to 4l}\)

Reimplemented from NPbase.

Definition at line 12660 of file NPSMEFTd6.cpp.

12661 {
12662  return muWH(sqrt_s) * BrHZZ4lRatio();
12663 
12664 }

◆ muZH()

double NPSMEFTd6::muZH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH}\)

Reimplemented from NPbase.

Definition at line 7033 of file NPSMEFTd6.cpp.

7034 {
7035  double mu = 1.0;
7036 
7037  double C1 = 0.0;
7038 
7039  if (sqrt_s == 1.96) {
7040 
7041  C1 = 0.0; // N.A.
7042 
7043  mu +=
7044  +121197. * (1. + eZH_2_Hbox ) * CiHbox / LambdaNP2
7045  -810445. * (1. + eZH_2_HQ1_11 ) * CiHQ1_11 / LambdaNP2
7046  +529340. * (1. + eZH_2_Hu_11 ) * CiHu_11 / LambdaNP2
7047  -69410.3 * (1. + eZH_2_Hd_11 ) * CiHd_11 / LambdaNP2
7048  +1567161. * (1. + eZH_2_HQ3_11 ) * CiHQ3_11 / LambdaNP2
7049  -16992.5 * (1. + eZH_2_HD ) * CiHD / LambdaNP2
7050  +79314.5 * (1. + eZH_2_HB ) * CiHB / LambdaNP2
7051  +711710. * (1. + eZH_2_HW ) * CiHW / LambdaNP2
7052  +189054. * (1. + eZH_2_HWB ) * CiHWB / LambdaNP2
7053  +9774.73 * (1. + eZH_2_DHB ) * CiDHB / LambdaNP2
7054  +130777. * (1. + eZH_2_DHW ) * CiDHW / LambdaNP2
7055  -2.535 * (1. + eZH_2_DeltaGF ) * DeltaGF()
7056  ;
7057 
7058  if (FlagQuadraticTerms) {
7059  //Add contributions that are quadratic in the effective coefficients
7060  mu += 0.0;
7061 
7062  }
7063 
7064  } else if (sqrt_s == 7.0) {
7065 
7066  C1 = 0.0123;
7067 
7068  mu +=
7069  +121069. * (1. + eZH_78_Hbox ) * CiHbox / LambdaNP2
7070  -182215. * (1. + eZH_78_HQ1_11 ) * CiHQ1_11 / LambdaNP2
7071  +421780. * (1. + eZH_78_Hu_11 ) * CiHu_11 / LambdaNP2
7072  -139169. * (1. + eZH_78_Hd_11 ) * CiHd_11 / LambdaNP2
7073  +1712111. * (1. + eZH_78_HQ3_11 ) * CiHQ3_11 / LambdaNP2
7074  -15395.4 * (1. + eZH_78_HD ) * CiHD / LambdaNP2
7075  +87094.9 * (1. + eZH_78_HB ) * CiHB / LambdaNP2
7076  +717388. * (1. + eZH_78_HW ) * CiHW / LambdaNP2
7077  +203105. * (1. + eZH_78_HWB ) * CiHWB / LambdaNP2
7078  +17532.4 * (1. + eZH_78_DHB ) * CiDHB / LambdaNP2
7079  +152950. * (1. + eZH_78_DHW ) * CiDHW / LambdaNP2
7080  -2.502 * (1. + eZH_78_DeltaGF ) * DeltaGF()
7081  ;
7082 
7083  if (FlagQuadraticTerms) {
7084  //Add contributions that are quadratic in the effective coefficients
7085  mu += 0.0;
7086 
7087  }
7088 
7089  } else if (sqrt_s == 8.0) {
7090 
7091  C1 = 0.0122;
7092 
7093  mu +=
7094  +121334. * (1. + eZH_78_Hbox ) * CiHbox / LambdaNP2
7095  -176804. * (1. + eZH_78_HQ1_11 ) * CiHQ1_11 / LambdaNP2
7096  +428587. * (1. + eZH_78_Hu_11 ) * CiHu_11 / LambdaNP2
7097  -142508. * (1. + eZH_78_Hd_11 ) * CiHd_11 / LambdaNP2
7098  +1747367. * (1. + eZH_78_HQ3_11 ) * CiHQ3_11 / LambdaNP2
7099  -15002.7 * (1. + eZH_78_HD ) * CiHD / LambdaNP2
7100  +87781.5 * (1. + eZH_78_HB ) * CiHB / LambdaNP2
7101  +721405. * (1. + eZH_78_HW ) * CiHW / LambdaNP2
7102  +204540. * (1. + eZH_78_HWB ) * CiHWB / LambdaNP2
7103  +18868.6 * (1. + eZH_78_DHB ) * CiDHB / LambdaNP2
7104  +158432. * (1. + eZH_78_DHW ) * CiDHW / LambdaNP2
7105  -2.507 * (1. + eZH_78_DeltaGF ) * DeltaGF()
7106  ;
7107 
7108  if (FlagQuadraticTerms) {
7109  //Add contributions that are quadratic in the effective coefficients
7110  mu += 0.0;
7111 
7112  }
7113 
7114  } else if (sqrt_s == 13.0) {
7115 
7116  C1 = 0.0119;
7117 
7118  mu +=
7119  +121374. * (1. + eZH_1314_Hbox ) * CiHbox / LambdaNP2
7120  -152273. * (1. + eZH_1314_HQ1_11 ) * CiHQ1_11 / LambdaNP2
7121  +448168. * (1. + eZH_1314_Hu_11 ) * CiHu_11 / LambdaNP2
7122  -155999. * (1. + eZH_1314_Hd_11 ) * CiHd_11 / LambdaNP2
7123  +1862364. * (1. + eZH_1314_HQ3_11 ) * CiHQ3_11 / LambdaNP2
7124  -15185. * (1. + eZH_1314_HD ) * CiHD / LambdaNP2
7125  +88937.9 * (1. + eZH_1314_HB ) * CiHB / LambdaNP2
7126  +728207. * (1. + eZH_1314_HW ) * CiHW / LambdaNP2
7127  +207857. * (1. + eZH_1314_HWB ) * CiHWB / LambdaNP2
7128  +21647.4 * (1. + eZH_1314_DHB ) * CiDHB / LambdaNP2
7129  +175015. * (1. + eZH_1314_DHW ) * CiDHW / LambdaNP2
7130  -2.506 * (1. + eZH_1314_DeltaGF ) * DeltaGF()
7131  ;
7132 
7133  if (FlagQuadraticTerms) {
7134  //Add contributions that are quadratic in the effective coefficients
7135  mu += 0.0;
7136 
7137  }
7138 
7139  } else if (sqrt_s == 14.0) {
7140 
7141  C1 = 0.0118;
7142 
7143  mu +=
7144  +121437. * (1. + eZH_1314_Hbox ) * CiHbox / LambdaNP2
7145  -147580. * (1. + eZH_1314_HQ1_11 ) * CiHQ1_11 / LambdaNP2
7146  +450628. * (1. + eZH_1314_Hu_11 ) * CiHu_11 / LambdaNP2
7147  -157625. * (1. + eZH_1314_Hd_11 ) * CiHd_11 / LambdaNP2
7148  +1878132. * (1. + eZH_1314_HQ3_11 ) * CiHQ3_11 / LambdaNP2
7149  -15299.4 * (1. + eZH_1314_HD ) * CiHD / LambdaNP2
7150  +88761.8 * (1. + eZH_1314_HB ) * CiHB / LambdaNP2
7151  +729243. * (1. + eZH_1314_HW ) * CiHW / LambdaNP2
7152  +207707. * (1. + eZH_1314_HWB ) * CiHWB / LambdaNP2
7153  +21958.9 * (1. + eZH_1314_DHB ) * CiDHB / LambdaNP2
7154  +177300. * (1. + eZH_1314_DHW ) * CiDHW / LambdaNP2
7155  -2.507 * (1. + eZH_1314_DeltaGF ) * DeltaGF()
7156  ;
7157 
7158  if (FlagQuadraticTerms) {
7159  //Add contributions that are quadratic in the effective coefficients
7160  mu += 0.0;
7161 
7162  }
7163 
7164  } else if (sqrt_s == 27.0) {
7165 
7166  C1 = 0.0116; // From arXiv: 1902.00134
7167 
7168  mu +=
7169  +121206. * CiHbox / LambdaNP2
7170  -101865. * CiHQ1_11 / LambdaNP2
7171  +468029. * CiHu_11 / LambdaNP2
7172  -173377. * CiHd_11 / LambdaNP2
7173  +2002478. * CiHQ3_11 / LambdaNP2
7174  -15486.3 * CiHD / LambdaNP2
7175  +89958. * CiHB / LambdaNP2
7176  +735013. * CiHW / LambdaNP2
7177  +211026. * CiHWB / LambdaNP2
7178  +25604. * CiDHB / LambdaNP2
7179  +196710. * CiDHW / LambdaNP2
7180  -2.505 * DeltaGF()
7181  ;
7182 
7183  if (FlagQuadraticTerms) {
7184  //Add contributions that are quadratic in the effective coefficients
7185  mu += 0.0;
7186 
7187  }
7188 
7189  } else if (sqrt_s == 100.0) {
7190 
7191  C1 = 0.0; // N.A.
7192 
7193  mu +=
7194  +121269. * CiHbox / LambdaNP2
7195  +90.68 * CiHQ1_11 / LambdaNP2
7196  +484275. * CiHu_11 / LambdaNP2
7197  -197878. * CiHd_11 / LambdaNP2
7198  +2175601. * CiHQ3_11 / LambdaNP2
7199  -14992.4 * CiHD / LambdaNP2
7200  +91707.3 * CiHB / LambdaNP2
7201  +741805. * CiHW / LambdaNP2
7202  +215319. * CiHWB / LambdaNP2
7203  +31435.6 * CiDHB / LambdaNP2
7204  +223843. * CiDHW / LambdaNP2
7205  -2.504 * DeltaGF()
7206  ;
7207 
7208  if (FlagQuadraticTerms) {
7209  //Add contributions that are quadratic in the effective coefficients
7210  mu += 0.0;
7211  }
7212 
7213  } else
7214  throw std::runtime_error("Bad argument in NPSMEFTd6::muZH()");
7215 
7216  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
7217  mu += eZHint + eZHpar;
7218 
7219 // Linear contribution from Higgs self-coupling
7220  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
7221 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
7223 
7224  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
7225 
7226  return mu;
7227 }

◆ muZHbb()

double NPSMEFTd6::muZHbb ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,bb}\) between the ZH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,bb}\)

Reimplemented from NPbase.

Definition at line 12834 of file NPSMEFTd6.cpp.

12835 {
12836  return muZH(sqrt_s) * BrHbbRatio();
12837 
12838 }

◆ muZHgaga()

double NPSMEFTd6::muZHgaga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,\gamma\gamma}\) between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 12546 of file NPSMEFTd6.cpp.

12547 {
12548  return muZH(sqrt_s) * BrHgagaRatio();
12549 
12550 }

◆ muZHmumu()

double NPSMEFTd6::muZHmumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,\mu\mu}\) between the ZH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,\mu\mu}\)

Reimplemented from NPbase.

Definition at line 12762 of file NPSMEFTd6.cpp.

12763 {
12764  return muZH(sqrt_s) * BrHmumuRatio();
12765 
12766 }

◆ muZHtautau()

double NPSMEFTd6::muZHtautau ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,\tau\tau}\) between the ZH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,\tau\tau}\)

Reimplemented from NPbase.

Definition at line 12798 of file NPSMEFTd6.cpp.

12799 {
12800  return muZH(sqrt_s) * BrHtautauRatio();
12801 
12802 }

◆ muZHWW()

double NPSMEFTd6::muZHWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,WW}\) between the ZH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,WW}\)

Reimplemented from NPbase.

Definition at line 12690 of file NPSMEFTd6.cpp.

12691 {
12692  return muZH(sqrt_s) * BrHWWRatio();
12693 
12694 }

◆ muZHWW2l2v()

double NPSMEFTd6::muZHWW2l2v ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,WW\to 2l2\nu}\) between the ZH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,WW\to 2l2\nu}\)

Reimplemented from NPbase.

Definition at line 12726 of file NPSMEFTd6.cpp.

12727 {
12728  return muZH(sqrt_s) * BrHWW2l2vRatio();
12729 
12730 }

◆ muZHZga()

double NPSMEFTd6::muZHZga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,Z\gamma}\) between the ZH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,Z\gamma}\)

Reimplemented from NPbase.

Definition at line 12582 of file NPSMEFTd6.cpp.

12583 {
12584  return muZH(sqrt_s) * BrHZgaRatio();
12585 
12586 }

◆ muZHZZ()

double NPSMEFTd6::muZHZZ ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,ZZ}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,ZZ}\)

Reimplemented from NPbase.

Definition at line 12618 of file NPSMEFTd6.cpp.

12619 {
12620  return muZH(sqrt_s) * BrHZZRatio();
12621 
12622 }

◆ muZHZZ4l()

double NPSMEFTd6::muZHZZ4l ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,ZZ\to 4l}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,ZZ\to 4l}\)

Reimplemented from NPbase.

Definition at line 12654 of file NPSMEFTd6.cpp.

12655 {
12656  return muZH(sqrt_s) * BrHZZ4lRatio();
12657 
12658 }

◆ Mw()

double NPSMEFTd6::Mw ( ) const
virtual

The mass of the \(W\) boson, \(M_W\).

Returns
\(M_W\) in GeV

Reimplemented from NPbase.

Definition at line 2743 of file NPSMEFTd6.cpp.

2744 {
2745  return (trueSM.Mw() - Mw_tree() / 4.0 / (cW2_tree - sW2_tree)
2746  *(4.0 * sW_tree * cW_tree * CiHWB * v2_over_LambdaNP2
2748  + 2.0 * sW2_tree * DeltaGF()));
2749 }

◆ obliqueS()

double NPSMEFTd6::obliqueS ( ) const
virtual

The oblique parameter \(S\). (Simplified implementation. Contribution only from \(O_{HWB}\).)

Returns
the value of \(S\)

Reimplemented from NPbase.

Definition at line 2603 of file NPSMEFTd6.cpp.

2604 {
2605  return (4.0 * sW_tree * cW_tree * CiHWB / alphaMz() * v2_over_LambdaNP2);
2606 }

◆ obliqueT()

double NPSMEFTd6::obliqueT ( ) const
virtual

The oblique parameter \(T\). (Simplified implementation. Contribution only from \(O_{HD}\).)

Returns
the value of \(T\)

Reimplemented from NPbase.

Definition at line 2608 of file NPSMEFTd6.cpp.

2609 {
2610  return (-CiHD / 2.0 / alphaMz() * v2_over_LambdaNP2);
2611 }

◆ obliqueU()

double NPSMEFTd6::obliqueU ( ) const
virtual

The oblique parameter \(U\).

Returns
the value of \(U\)

Reimplemented from NPbase.

Definition at line 2613 of file NPSMEFTd6.cpp.

2614 {
2615  return 0.0;
2616 }

◆ obliqueW()

double NPSMEFTd6::obliqueW ( ) const
virtual

The oblique parameter \(W\). (Simplified implementation. Contribution only from \(O_{2W}\).)

Returns
the value of \(W\)

Reimplemented from NPbase.

Definition at line 2618 of file NPSMEFTd6.cpp.

2619 {
2620  return (- g2_tree * g2_tree * (C2W + 0.5 * C2WS) * v2_over_LambdaNP2 / 2.0);
2621 }

◆ obliqueY()

double NPSMEFTd6::obliqueY ( ) const
virtual

The oblique parameter \(Y\). (Simplified implementation. Contribution only from \(O_{2B}\).)

Returns
the value of \(Y\)

Reimplemented from NPbase.

Definition at line 2623 of file NPSMEFTd6.cpp.

2624 {
2625  return (- g2_tree * g2_tree * (C2B + 0.5 * C2BS) * v2_over_LambdaNP2 / 2.0);
2626 }

◆ PostUpdate()

bool NPSMEFTd6::PostUpdate ( )
virtual

The post-update method for NPSMEFTd6.

This method runs all the procedures that are need to be executed after the model is successfully updated.

Returns
a boolean that is true if the execution is successful

Reimplemented from NPbase.

Definition at line 863 of file NPSMEFTd6.cpp.

864 {
865  if (!NPbase::PostUpdate()) return (false);
866 
867 // 0) Post-update operations not involving SM nor NP parameters
868  if (!FlagHiggsSM) {
869  cHSM = 0.0;
870  } else {
871  cHSM = 1.0;
872  }
873 
874  if (!FlagLoopHd6) {
875  cLHd6 = 0.0;
876  } else {
877  cLHd6 = 1.0;
878  }
879 
881  cLH3d62 = 1.0;
882  } else {
883  cLH3d62 = 0.0;
884  }
885 
886 // 1) Post-update operations involving SM parameters only
888  v2 = v() * v();
890  aleMz = alphaMz();
891  eeMz = sqrt( 4.0 * M_PI * aleMz );
892  eeMz2 = eeMz*eeMz;
893  cW_tree = Mw_tree() / Mz;
895  sW2_tree = 1.0 - cW2_tree;
896  sW_tree = sqrt(sW2_tree);
897 
898  g1_tree = eeMz/cW_tree;
899  g2_tree = eeMz/sW_tree;
900  g3_tree = sqrt( 4.0 * M_PI * AlsMz );
901 
902  lambdaH_tree = mHl*mHl/2.0/v2;
903 
905  gZlL = (leptons[ELECTRON].getIsospin()) - (leptons[ELECTRON].getCharge())*sW2_tree;
907  gZuL = (quarks[UP].getIsospin()) - (quarks[UP].getCharge())*sW2_tree;
908  gZuR = - (quarks[UP].getCharge()) * sW2_tree;
909  gZdL = (quarks[DOWN].getIsospin()) - (quarks[DOWN].getCharge())*sW2_tree;
910  gZdR = - (quarks[DOWN].getCharge()) * sW2_tree;
911 
912  UevL = 1.0; // Neglect PMNS effects
913  VudL = 1.0; // Neglect CKM effects
914 
915  Yuke = sqrt(2.) * (leptons[ELECTRON].getMass()) / v();
916  Yukmu = sqrt(2.) * (leptons[MU].getMass()) / v();
917  Yuktau = sqrt(2.) * (leptons[TAU].getMass()) / v();
918  Yuku = sqrt(2.) * (quarks[UP].getMass()) / v();
919  Yukc = sqrt(2.) * (quarks[CHARM].getMass()) / v();
920  Yukt = sqrt(2.) * mtpole / v();
921  Yukd = sqrt(2.) * (quarks[DOWN].getMass()) / v();
922  Yuks = sqrt(2.) * (quarks[STRANGE].getMass()) / v();
923  Yukb = sqrt(2.) * (quarks[BOTTOM].getMass()) / v();
924 
925  dZH = -(9.0/16.0)*( GF*mHl*mHl/sqrt(2.0)/M_PI/M_PI )*( 2.0*M_PI/3.0/sqrt(3.0) - 1.0 );
926 
927 // 2) Post-update operations related to assumptions in the form of the dimension-6 operators
928 
929 // Rotated CHW and CHB parameters: Here I need to overwrite the model parameters (There are always 2 on/2 off but need the values of both in output)
930  if (FlagRotateCHWCHB) {
933  } else {
936  }
937 
938 // Flavour universality assumptions
939 
940 // Initialize the internal Wilson coeffs of the form CfH and CfV from the model parameters
941  CieH_11r = CeH_11r;
942  CieH_22r = CeH_22r;
943  CieH_33r = CeH_33r;
944 
945  CiuH_11r = CuH_11r;
946  CiuH_22r = CuH_22r;
947  CiuH_33r = CuH_33r;
948 
949  CidH_11r = CdH_11r;
950  CidH_22r = CdH_22r;
951  CidH_33r = CdH_33r;
952 
953  CiuG_11r = CuG_11r;
954  CiuG_22r = CuG_22r;
955  CiuG_33r = CuG_33r;
956 
957  CiuW_11r = CuW_11r;
958  CiuW_22r = CuW_22r;
959  CiuW_33r = CuW_33r;
960 
961  CiuB_11r = CuB_11r;
962  CiuB_22r = CuB_22r;
963  CiuB_33r = CuB_33r;
964 
965 // and depending on the flavour assumptions rewrite the values (but never rewritting the values model parameters)
966 
967  if (FlagFlavU3OfX || FlagUnivOfX) {
968 
969  if (FlagUnivOfX) {
970 // All equal to uH_33r
971  CieH_11r = CuH_33r;
972  CieH_22r = CuH_33r;
973  CieH_33r = CuH_33r;
974 
975  CiuH_11r = CuH_33r;
976  CiuH_22r = CuH_33r;
977  // CiuH_33r = CuH_33r;
978 
979  CidH_11r = CuH_33r;
980  CidH_22r = CuH_33r;
981  CidH_33r = CuH_33r;
982 
983  // Currently OfV are only implemented for u quarks so nothing else is needed to apply universality.
984  }
985 
986 // Proportional to Yukawa interactions Wilson coeff in Warsaw - C=y c - Wilson coeff in model par
987 
988  CieH_11r = Yuke * CeH_11r;
989  CieH_22r = Yukmu * CeH_22r;
990  CieH_33r = Yuktau * CeH_33r;
991 
992  CiuH_11r = Yuku * CuH_11r;
993  CiuH_22r = Yukc * CuH_22r;
994  CiuH_33r = Yukt * CuH_33r;
995 
996  CidH_11r = Yukd * CdH_11r;
997  CidH_22r = Yuks * CdH_22r;
998  CidH_33r = Yukb * CdH_33r;
999 
1000  CiuG_11r = Yuku * CuG_11r;
1001  CiuG_22r = Yukc * CuG_22r;
1002  CiuG_33r = Yukt * CuG_33r;
1003 
1004  CiuW_11r = Yuku * CuW_11r;
1005  CiuW_22r = Yukc * CuW_22r;
1006  CiuW_33r = Yukt * CuW_33r;
1007 
1008  CiuB_11r = Yuku * CuB_11r;
1009  CiuB_22r = Yukc * CuB_22r;
1010  CiuB_33r = Yukt * CuB_33r;
1011  }
1012 
1013 // C2B, C2W, C2WS, C2BS, CDB, CDW, CT are incorporated by change of basis transformation:
1014 // Write here, before working with the dim 6 interactions,
1015 // the contributions from O2W and O2B to the other operators.
1016 // WARNING: Ignoring contributions to 4 fermion-processes for the moment. IMPORTANT FOR LEP2
1017 
1018 // WARNING (OBSOLETE MESSAGE?): if some of the parameters below, e.g. CHL1_11, are not floating in the fit this will
1019 // create a problem since the value generated below CHL1_11 will propagate to the next iteration
1020 // generating an uncontrolled value of the parameter.
1021 // (This is so because SetParameters is not called for non-floating parameters.)
1022 // Possible fix: Not modify model parameters but save everything into internal replicas
1023 // of each model relevant model par. Those then have to be used in the calculations.
1024 // Comment out the following lines until this is resolved
1025 
1026 // Contributionsfrom C2W, C2B, C2WS, C2BS, CT
1027  CiHL1_11 = CHL1_11 - (g1_tree*g1_tree/2.0) * (C2B + 0.5 * C2BS);
1028  CiHL1_22 = CHL1_22 - (g1_tree*g1_tree/2.0) * (C2B + 0.5 * C2BS);
1029  CiHL1_33 = CHL1_33 - (g1_tree*g1_tree/2.0) * (C2B + 0.5 * C2BS);
1030  CiHL3_11 = CHL3_11 + (g2_tree*g2_tree/2.0) * (C2W + 0.5 * C2WS);
1031  CiHL3_22 = CHL3_22 + (g2_tree*g2_tree/2.0) * (C2W + 0.5 * C2WS);
1032  CiHL3_33 = CHL3_33 + (g2_tree*g2_tree/2.0) * (C2W + 0.5 * C2WS);
1033 
1034  CiHQ1_11 = CHQ1_11 + (g1_tree*g1_tree/6.0) * (C2B + 0.5 * C2BS);
1035  CiHQ1_22 = CHQ1_22 + (g1_tree*g1_tree/6.0) * (C2B + 0.5 * C2BS);
1036  CiHQ1_33 = CHQ1_33 + (g1_tree*g1_tree/6.0) * (C2B + 0.5 * C2BS);
1037  CiHQ3_11 = CHQ3_11 + (g2_tree*g2_tree/2.0) * (C2W + 0.5 * C2WS);
1038  CiHQ3_22 = CHQ3_22 + (g2_tree*g2_tree/2.0) * (C2W + 0.5 * C2WS);
1039  CiHQ3_33 = CHQ3_33 + (g2_tree*g2_tree/2.0) * (C2W + 0.5 * C2WS);
1040 
1041  CiHe_11 = CHe_11 - (g1_tree*g1_tree) * (C2B + 0.5 * C2BS);
1042  CiHe_22 = CHe_22 - (g1_tree*g1_tree) * (C2B + 0.5 * C2BS);
1043  CiHe_33 = CHe_33 - (g1_tree*g1_tree) * (C2B + 0.5 * C2BS);
1044 
1045  CiHu_11 = CHu_11 + (2.0*g1_tree*g1_tree/3.0) * (C2B + 0.5 * C2BS);
1046  CiHu_22 = CHu_22 + (2.0*g1_tree*g1_tree/3.0) * (C2B + 0.5 * C2BS);
1047  CiHu_33 = CHu_33 + (2.0*g1_tree*g1_tree/3.0) * (C2B + 0.5 * C2BS);
1048 
1049  CiHd_11 = CHd_11 - (g1_tree*g1_tree/3.0) * (C2B + 0.5 * C2BS);
1050  CiHd_22 = CHd_22 - (g1_tree*g1_tree/3.0) * (C2B + 0.5 * C2BS);
1051  CiHd_33 = CHd_33 - (g1_tree*g1_tree/3.0) * (C2B + 0.5 * C2BS);
1052 
1053  CiW = CW + g2_tree * C2W;
1054 
1055  CiHbox = CHbox - 0.5 * CT + (g1_tree*g1_tree/4.0) * (C2B + 0.5 * C2BS) + (3.0*g2_tree*g2_tree/4.0) * (C2W + 0.5 * C2WS);
1056  CiHD = CHD - 2.0 * CT + (g1_tree*g1_tree/4.0) * (C2B + 0.5 * C2BS);
1057  CiH = CH + (2.0*g2_tree*g2_tree*lambdaH_tree) * (C2W + 0.5 * C2WS);
1058 
1059 // For the CfH I must use CifH = CifH + ... to account for previous operations.
1060 
1061  CieH_11r = CieH_11r + (g2_tree*g2_tree*Yuke) * (C2W + 0.5 * C2WS);
1062  CieH_22r = CieH_22r + (g2_tree*g2_tree*Yukmu) * (C2W + 0.5 * C2WS);
1063  CieH_33r = CieH_33r + (g2_tree*g2_tree*Yuktau) * (C2W + 0.5 * C2WS);
1064 
1065  CiuH_11r = CiuH_11r + (g2_tree*g2_tree*Yuku) * (C2W + 0.5 * C2WS);
1066  CiuH_22r = CiuH_22r + (g2_tree*g2_tree*Yukc) * (C2W + 0.5 * C2WS);
1067  CiuH_33r = CiuH_33r + (g2_tree*g2_tree*Yukt) * (C2W + 0.5 * C2WS);
1068 
1069  CidH_11r = CidH_11r + (g2_tree*g2_tree*Yukd) * (C2W + 0.5 * C2WS);
1070  CidH_22r = CidH_22r + (g2_tree*g2_tree*Yuks) * (C2W + 0.5 * C2WS);
1071  CidH_33r = CidH_33r + (g2_tree*g2_tree*Yukb) * (C2W + 0.5 * C2WS);
1072 
1073  CiLL_1221 = CLL_1221 + (g2_tree*g2_tree/2.0) * (C2W + 0.5 * C2WS);
1074  CiLL_2112 = CiLL_1221;
1075 
1076 // Contributionsfrom CDW, DB
1077  CiHB = CHB + (g1_tree/4.0) * CDB;
1078  CiHW = CHW + (g2_tree/4.0) * CDW;
1079 // CiHWHB_gaga = CHWHB_gaga;
1080 // CiHWHB_gagaorth = CHWHB_gagaorth;
1081  CiDHB = CDHB + CDB;
1082  CiDHW = CDHW + CDW;
1083  CiHWB = CHWB + (1.0/4.0) * ( g1_tree * CDW + g2_tree * CDB );
1084 
1085 // 3) Post-update operations working directly with the dimension six operators
1086 
1091  delta_h = (-CiHD / 4.0 + CiHbox) * v2_over_LambdaNP2;
1092 
1093 // Calculation of some quantities repeteadly used in the code
1094 
1095 // NP corrections to Total Higgs width
1097 
1098  if (FlagQuadraticTerms) {
1100  } else {
1101  dGammaHTotR2 = 0.0;
1102  }
1103 
1104 // Total: to be used in BR functions to check positivity
1106 
1107  // The total theory error in the H width: set to 0.0 for the moment
1109 
1110 // Dimension-6 coefficients used in the STXS parameterization
1111  aiG = 16.0 * M_PI * M_PI * CHG * Mw_tree() * Mw_tree() / g3_tree / g3_tree / LambdaNP2;
1112  ai3G = CG * Mw_tree() * Mw_tree() / g3_tree / g3_tree / g3_tree / LambdaNP2;
1113  ai2G =0.0; // Add
1114  aiT = 2.0 * CiHD * v2_over_LambdaNP2;
1115  aiH = - 2.0 * CiHbox * v2_over_LambdaNP2;
1116  aiWW = 0.0; // Add
1117  aiB = 0.0; // Add
1118  aiHW = CiDHW * Mw_tree() * Mw_tree() / 2.0 / g2_tree / LambdaNP2;
1119  aiHB = CiDHB * Mw_tree() * Mw_tree() / 2.0 / g1_tree / LambdaNP2;
1120  aiA = CiHB * Mw_tree() * Mw_tree() / g1_tree / g1_tree / LambdaNP2;
1121  aiHQ = CiHQ1_11 * v2_over_LambdaNP2; // Valid only for flavour universal NP
1122  aipHQ = CiHQ3_11 * v2_over_LambdaNP2; // Valid only for flavour universal NP
1123  aiHL = CiHL1_11 * v2_over_LambdaNP2; // Valid only for flavour universal NP
1124  aipHL = CiHL3_11 * v2_over_LambdaNP2; // Valid only for flavour universal NP. From HEL Lagrangian. Not in original note
1125  aiHu = CiHu_11 * v2_over_LambdaNP2; // Valid only for flavour universal NP
1126  aiHd = CiHd_11 * v2_over_LambdaNP2; // Valid only for flavour universal NP
1127  aiHe = CiHe_11 * v2_over_LambdaNP2; // Valid only for flavour universal NP
1129  aiuG = CiuG_33r * Mw_tree() * Mw_tree() / g3_tree / LambdaNP2 / Yukt / 4.0; // From HEL.fr Lagrangian. Not in original note. Valid only for flavour universal NP
1130 
1131 
1132 // Dim 6 SMEFT matching
1133 
1135 
1136  return (true);
1137 }

◆ ppZHprobe()

double NPSMEFTd6::ppZHprobe ( const double  sqrt_s) const
virtual

The direction constrained by \( p p \to Z H\) in the boosted regime, \(g_p^Z\). From arXiv:1807.01796 and the contribution to FCC CDR Vol 1. Implemented only in NPSMEFTd6 class.

Returns
\(g_p^Z\)

Reimplemented from NPbase.

Definition at line 14575 of file NPSMEFTd6.cpp.

14576 {
14577 
14578  double gpZ=0.0;
14579 
14580  double ghZuL,ghZdL,ghZuR,ghZdR;
14581 
14582  // In the Warsaw basis the contact interactions are generated only by CHF ops but
14583  // in the modified basis ODHB, ODHW also contribute
14584 
14585  ghZuL = -(eeMz/sW_tree/cW_tree)*(CiHQ1_11 - CiHQ3_11 + g1_tree * (1.0/12.0) * CiDHB - (g2_tree/4.0) * CiDHW) * v2_over_LambdaNP2;
14586  ghZdL = -(eeMz/sW_tree/cW_tree)*(CiHQ1_11 + CiHQ3_11 + g1_tree * (1.0/12.0) * CiDHB + (g2_tree/4.0) * CiDHW) * v2_over_LambdaNP2;
14587  ghZuR = -(eeMz/sW_tree/cW_tree)*(CiHu_11 + g1_tree * (1.0/3.0) * CiDHB) * v2_over_LambdaNP2;
14588  ghZdR = -(eeMz/sW_tree/cW_tree)*(CiHd_11 - g1_tree * (1.0/6.0) * CiDHB) * v2_over_LambdaNP2;
14589 
14590  if (sqrt_s == 14.0) {
14591 
14592  gpZ = ghZuL - 0.76 * ghZdL - 0.45 * ghZuR + 0.14 * ghZdR;
14593 
14594  } else if (sqrt_s == 27.0) {
14595  // Use the same as for 14 TeV for the moment
14596 
14597  gpZ = ghZuL - 0.76 * ghZdL - 0.45 * ghZuR + 0.14 * ghZdR;
14598 
14599  } else if (sqrt_s == 100.0) {
14600 
14601  gpZ = ghZuL - 0.90 * ghZdL - 0.45 * ghZuR + 0.17 * ghZdR;
14602 
14603  } else
14604  throw std::runtime_error("Bad argument in NPSMEFTd6::ppZHprobe()");
14605 
14606 
14607  return gpZ;
14608 
14609 }

◆ setFlag()

bool NPSMEFTd6::setFlag ( const std::string  name,
const bool  value 
)
virtual

A method to set a flag of NPSMEFTd6.

Parameters
[in]namename of a model flag
[in]valuethe boolean to be assigned to the flag specified by name
Returns
a boolean that is true if the execution is successful

Reimplemented from StandardModel.

Definition at line 2377 of file NPSMEFTd6.cpp.

2378 {
2379  bool res = false;
2380  if (name.compare("QuadraticTerms") == 0) {
2381  FlagQuadraticTerms = value;
2382  if(value) setModelLinearized(false);
2383  res = true;
2384  } else if (name.compare("RotateCHWCHB") == 0) {
2385  FlagRotateCHWCHB = value;
2386  res = true;
2387  } else if (name.compare("PartialQFU") == 0) {
2388  FlagPartialQFU = value;
2389  res = true;
2390  } else if (name.compare("FlavU3OfX") == 0) {
2391  FlagFlavU3OfX = value;
2392  res = true;
2393  } else if (name.compare("UnivOfX") == 0) {
2394  FlagUnivOfX = value;
2395  res = true;
2396  } else if (name.compare("HiggsSM") == 0) {
2397  FlagHiggsSM = value;
2398  res = true;
2399  } else if (name.compare("LoopHd6") == 0) {
2400  FlagLoopHd6 = value;
2401  res = true;
2402  } else if (name.compare("LoopH3d6Quad") == 0) {
2403  FlagLoopH3d6Quad = value;
2404  res = true;
2405  } else
2406  res = NPbase::setFlag(name, value);
2407 
2408  return (res);
2409 }

◆ setParameter()

void NPSMEFTd6::setParameter ( const std::string  name,
const double &  value 
)
protectedvirtual

A method to set the value of a parameter of the model.

Parameters
[in]namename of a model parameter
[in]valuethe value to be assigned to the parameter specified by name

Reimplemented from StandardModel.

Definition at line 1139 of file NPSMEFTd6.cpp.

1140 {
1141  if (name.compare("CG") == 0)
1142  CG = value;
1143  else if (name.compare("CW") == 0)
1144  CW = value;
1145  else if (name.compare("C2B") == 0)
1146  C2B = value;
1147  else if (name.compare("C2W") == 0)
1148  C2W = value;
1149  else if (name.compare("C2BS") == 0)
1150  C2BS = value;
1151  else if (name.compare("C2WS") == 0)
1152  C2WS = value;
1153  else if (name.compare("CHG") == 0)
1154  CHG = value;
1155  else if (name.compare("CHW") == 0)
1156  CHW = value;
1157  else if (name.compare("CHB") == 0)
1158  CHB = value;
1159  else if (name.compare("CHWHB_gaga") == 0)
1160  CHWHB_gaga = value;
1161  else if (name.compare("CHWHB_gagaorth") == 0)
1162  CHWHB_gagaorth = value;
1163  else if (name.compare("CDHB") == 0)
1164  CDHB = value;
1165  else if (name.compare("CDHW") == 0)
1166  CDHW = value;
1167  else if (name.compare("CDB") == 0)
1168  CDB = value;
1169  else if (name.compare("CDW") == 0)
1170  CDW = value;
1171  else if (name.compare("CHWB") == 0)
1172  CHWB = value;
1173  else if (name.compare("CHD") == 0)
1174  CHD = value;
1175  else if (name.compare("CT") == 0)
1176  CT = value;
1177  else if (name.compare("CHbox") == 0)
1178  CHbox = value;
1179  else if (name.compare("CH") == 0)
1180  CH = value;
1181  else if (name.compare("CHL1_11") == 0)
1182  CHL1_11 = value;
1183  else if (name.compare("CHL1_12r") == 0)
1184  CHL1_12r = value;
1185  else if (name.compare("CHL1_13r") == 0)
1186  CHL1_13r = value;
1187  else if (name.compare("CHL1_22") == 0)
1188  CHL1_22 = value;
1189  else if (name.compare("CHL1_23r") == 0)
1190  CHL1_23r = value;
1191  else if (name.compare("CHL1_33") == 0)
1192  CHL1_33 = value;
1193  else if (name.compare("CHL1_12i") == 0)
1194  CHL1_12i = value;
1195  else if (name.compare("CHL1_13i") == 0)
1196  CHL1_13i = value;
1197  else if (name.compare("CHL1_23i") == 0)
1198  CHL1_23i = value;
1199  else if (name.compare("CHL1") == 0) {
1200  CHL1_11 = value;
1201  CHL1_12r = 0.0;
1202  CHL1_13r = 0.0;
1203  CHL1_22 = value;
1204  CHL1_23r = 0.0;
1205  CHL1_33 = value;
1206  CHL1_12i = 0.0;
1207  CHL1_13i = 0.0;
1208  CHL1_23i = 0.0;
1209  } else if (name.compare("CHL3_11") == 0)
1210  CHL3_11 = value;
1211  else if (name.compare("CHL3_12r") == 0)
1212  CHL3_12r = value;
1213  else if (name.compare("CHL3_13r") == 0)
1214  CHL3_13r = value;
1215  else if (name.compare("CHL3_22") == 0)
1216  CHL3_22 = value;
1217  else if (name.compare("CHL3_23r") == 0)
1218  CHL3_23r = value;
1219  else if (name.compare("CHL3_33") == 0)
1220  CHL3_33 = value;
1221  else if (name.compare("CHL3_12i") == 0)
1222  CHL3_12i = value;
1223  else if (name.compare("CHL3_13i") == 0)
1224  CHL3_13i = value;
1225  else if (name.compare("CHL3_23i") == 0)
1226  CHL3_23i = value;
1227  else if (name.compare("CHL3") == 0) {
1228  CHL3_11 = value;
1229  CHL3_12r = 0.0;
1230  CHL3_13r = 0.0;
1231  CHL3_22 = value;
1232  CHL3_23r = 0.0;
1233  CHL3_33 = value;
1234  CHL3_12i = 0.0;
1235  CHL3_13i = 0.0;
1236  CHL3_23i = 0.0;
1237  } else if (name.compare("CHe_11") == 0)
1238  CHe_11 = value;
1239  else if (name.compare("CHe_12r") == 0)
1240  CHe_12r = value;
1241  else if (name.compare("CHe_13r") == 0)
1242  CHe_13r = value;
1243  else if (name.compare("CHe_22") == 0)
1244  CHe_22 = value;
1245  else if (name.compare("CHe_23r") == 0)
1246  CHe_23r = value;
1247  else if (name.compare("CHe_33") == 0)
1248  CHe_33 = value;
1249  else if (name.compare("CHe_12i") == 0)
1250  CHe_12i = value;
1251  else if (name.compare("CHe_13i") == 0)
1252  CHe_13i = value;
1253  else if (name.compare("CHe_23i") == 0)
1254  CHe_23i = value;
1255  else if (name.compare("CHe") == 0) {
1256  CHe_11 = value;
1257  CHe_12r = 0.0;
1258  CHe_13r = 0.0;
1259  CHe_22 = value;
1260  CHe_23r = 0.0;
1261  CHe_33 = value;
1262  CHe_12i = 0.0;
1263  CHe_13i = 0.0;
1264  CHe_23i = 0.0;
1265  } else if (name.compare("CHQ1_11") == 0) {
1266  CHQ1_11 = value;
1267  if (FlagPartialQFU){
1268  CHQ1_22 = value;
1269  }
1270  } else if (name.compare("CHQ1_12r") == 0)
1271  CHQ1_12r = value;
1272  else if (name.compare("CHQ1_13r") == 0)
1273  CHQ1_13r = value;
1274  else if (name.compare("CHQ1_22") == 0) {
1275  if (!FlagPartialQFU){
1276  CHQ1_22 = value;
1277  }
1278  } else if (name.compare("CHQ1_23r") == 0)
1279  CHQ1_23r = value;
1280  else if (name.compare("CHQ1_33") == 0)
1281  CHQ1_33 = value;
1282  else if (name.compare("CHQ1_12i") == 0)
1283  CHQ1_12i = value;
1284  else if (name.compare("CHQ1_13i") == 0)
1285  CHQ1_13i = value;
1286  else if (name.compare("CHQ1_23i") == 0)
1287  CHQ1_23i = value;
1288  else if (name.compare("CHQ1") == 0) {
1289  CHQ1_11 = value;
1290  CHQ1_12r = 0.0;
1291  CHQ1_13r = 0.0;
1292  CHQ1_22 = value;
1293  CHQ1_23r = 0.0;
1294  CHQ1_33 = value;
1295  CHQ1_12i = 0.0;
1296  CHQ1_13i = 0.0;
1297  CHQ1_23i = 0.0;
1298  } else if (name.compare("CHQ3_11") == 0){
1299  CHQ3_11 = value;
1300  if (FlagPartialQFU){
1301  CHQ3_22 = value;
1302  }
1303  } else if (name.compare("CHQ3_12r") == 0)
1304  CHQ3_12r = value;
1305  else if (name.compare("CHQ3_13r") == 0)
1306  CHQ3_13r = value;
1307  else if (name.compare("CHQ3_22") == 0){
1308  if (!FlagPartialQFU){
1309  CHQ3_22 = value;
1310  }
1311  } else if (name.compare("CHQ3_23r") == 0)
1312  CHQ3_23r = value;
1313  else if (name.compare("CHQ3_33") == 0)
1314  CHQ3_33 = value;
1315  else if (name.compare("CHQ3_12i") == 0)
1316  CHQ3_12i = value;
1317  else if (name.compare("CHQ3_13i") == 0)
1318  CHQ3_13i = value;
1319  else if (name.compare("CHQ3_23i") == 0)
1320  CHQ3_23i = value;
1321  else if (name.compare("CHQ3") == 0) {
1322  CHQ3_11 = value;
1323  CHQ3_12r = 0.0;
1324  CHQ3_13r = 0.0;
1325  CHQ3_22 = value;
1326  CHQ3_23r = 0.0;
1327  CHQ3_33 = value;
1328  CHQ3_12i = 0.0;
1329  CHQ3_13i = 0.0;
1330  CHQ3_23i = 0.0;
1331  } else if (name.compare("CHu_11") == 0){
1332  CHu_11 = value;
1333  if (FlagPartialQFU){
1334  CHu_22 = value;
1335  }
1336  } else if (name.compare("CHu_12r") == 0)
1337  CHu_12r = value;
1338  else if (name.compare("CHu_13r") == 0)
1339  CHu_13r = value;
1340  else if (name.compare("CHu_22") == 0){
1341  if (!FlagPartialQFU){
1342  CHu_22 = value;
1343  }
1344  } else if (name.compare("CHu_23r") == 0)
1345  CHu_23r = value;
1346  else if (name.compare("CHu_33") == 0)
1347  CHu_33 = value;
1348  else if (name.compare("CHu_12i") == 0)
1349  CHu_12i = value;
1350  else if (name.compare("CHu_13i") == 0)
1351  CHu_13i = value;
1352  else if (name.compare("CHu_23i") == 0)
1353  CHu_23i = value;
1354  else if (name.compare("CHu") == 0) {
1355  CHu_11 = value;
1356  CHu_12r = 0.0;
1357  CHu_13r = 0.0;
1358  CHu_22 = value;
1359  CHu_23r = 0.0;
1360  CHu_33 = value;
1361  CHu_12i = 0.0;
1362  CHu_13i = 0.0;
1363  CHu_23i = 0.0;
1364  } else if (name.compare("CHd_11") == 0){
1365  CHd_11 = value;
1366  if (FlagPartialQFU){
1367  CHd_22 = value;
1368  }
1369  } else if (name.compare("CHd_12r") == 0)
1370  CHd_12r = value;
1371  else if (name.compare("CHd_13r") == 0)
1372  CHd_13r = value;
1373  else if (name.compare("CHd_22") == 0){
1374  if (!FlagPartialQFU){
1375  CHd_22 = value;
1376  }
1377  } else if (name.compare("CHd_23r") == 0)
1378  CHd_23r = value;
1379  else if (name.compare("CHd_33") == 0)
1380  CHd_33 = value;
1381  else if (name.compare("CHd_12i") == 0)
1382  CHd_12i = value;
1383  else if (name.compare("CHd_13i") == 0)
1384  CHd_13i = value;
1385  else if (name.compare("CHd_23i") == 0)
1386  CHd_23i = value;
1387  else if (name.compare("CHd") == 0) {
1388  CHd_11 = value;
1389  CHd_12r = 0.0;
1390  CHd_13r = 0.0;
1391  CHd_22 = value;
1392  CHd_23r = 0.0;
1393  CHd_33 = value;
1394  CHd_12i = 0.0;
1395  CHd_13i = 0.0;
1396  CHd_23i = 0.0;
1397  } else if (name.compare("CHud_11r") == 0){
1398  CHud_11r = value;
1399  if (FlagPartialQFU){
1400  CHud_22r = value;
1401  }
1402  } else if (name.compare("CHud_12r") == 0)
1403  CHud_12r = value;
1404  else if (name.compare("CHud_13r") == 0)
1405  CHud_13r = value;
1406  else if (name.compare("CHud_22r") == 0){
1407  if (!FlagPartialQFU){
1408  CHud_22r = value;
1409  }
1410  } else if (name.compare("CHud_23r") == 0)
1411  CHud_23r = value;
1412  else if (name.compare("CHud_33r") == 0)
1413  CHud_33r = value;
1414  else if (name.compare("CHud_r") == 0) {
1415  CHud_11r = value;
1416  CHud_12r = 0.0;
1417  CHud_13r = 0.0;
1418  CHud_22r = value;
1419  CHud_23r = 0.0;
1420  CHud_33r = value;
1421  } else if (name.compare("CHud_11i") == 0){
1422  CHud_11i = value;
1423  if (FlagPartialQFU){
1424  CHud_22i = value;
1425  }
1426  } else if (name.compare("CHud_12i") == 0)
1427  CHud_12i = value;
1428  else if (name.compare("CHud_13i") == 0)
1429  CHud_13i = value;
1430  else if (name.compare("CHud_22i") == 0){
1431  if (!FlagPartialQFU){
1432  CHud_22i = value;
1433  }
1434  } else if (name.compare("CHud_23i") == 0)
1435  CHud_23i = value;
1436  else if (name.compare("CHud_33i") == 0)
1437  CHud_33i = value;
1438  else if (name.compare("CHud_i") == 0) {
1439  CHud_11i = value;
1440  CHud_12i = 0.0;
1441  CHud_13i = 0.0;
1442  CHud_22i = value;
1443  CHud_23i = 0.0;
1444  CHud_33i = value;
1445  } else if (name.compare("CeH_11r") == 0){
1446  if (!FlagFlavU3OfX){
1447  CeH_11r = value;
1448  }
1449  } else if (name.compare("CeH_12r") == 0)
1450  CeH_12r = value;
1451  else if (name.compare("CeH_13r") == 0)
1452  CeH_13r = value;
1453  else if (name.compare("CeH_22r") == 0){
1454  if (!FlagFlavU3OfX){
1455  CeH_22r = value;
1456  }
1457  } else if (name.compare("CeH_23r") == 0)
1458  CeH_23r = value;
1459  else if (name.compare("CeH_33r") == 0){
1460  CeH_33r = value;
1461  if (FlagFlavU3OfX){
1462  CeH_11r = value;
1463  CeH_22r = value;
1464  }
1465  } else if (name.compare("CeH_11i") == 0)
1466  CeH_11i = value;
1467  else if (name.compare("CeH_12i") == 0)
1468  CeH_12i = value;
1469  else if (name.compare("CeH_13i") == 0)
1470  CeH_13i = value;
1471  else if (name.compare("CeH_22i") == 0)
1472  CeH_22i = value;
1473  else if (name.compare("CeH_23i") == 0)
1474  CeH_23i = value;
1475  else if (name.compare("CeH_33i") == 0)
1476  CeH_33i = value;
1477  else if (name.compare("CuH_11r") == 0){
1478  if (!FlagFlavU3OfX){
1479  CuH_11r = value;
1480  }
1481  } else if (name.compare("CuH_12r") == 0)
1482  CuH_12r = value;
1483  else if (name.compare("CuH_13r") == 0)
1484  CuH_13r = value;
1485  else if (name.compare("CuH_22r") == 0){
1486  if (!FlagFlavU3OfX){
1487  CuH_22r = value;
1488  }
1489  } else if (name.compare("CuH_23r") == 0)
1490  CuH_23r = value;
1491  else if (name.compare("CuH_33r") == 0){
1492  CuH_33r = value;
1493  if (FlagFlavU3OfX){
1494  CuH_11r = value;
1495  CuH_22r = value;
1496  }
1497  } else if (name.compare("CuH_11i") == 0)
1498  CuH_11i = value;
1499  else if (name.compare("CuH_12i") == 0)
1500  CuH_12i = value;
1501  else if (name.compare("CuH_13i") == 0)
1502  CuH_13i = value;
1503  else if (name.compare("CuH_22i") == 0)
1504  CuH_22i = value;
1505  else if (name.compare("CuH_23i") == 0)
1506  CuH_23i = value;
1507  else if (name.compare("CuH_33i") == 0)
1508  CuH_33i = value;
1509  else if (name.compare("CdH_11r") == 0){
1510  if (!FlagFlavU3OfX){
1511  CdH_11r = value;
1512  }
1513  } else if (name.compare("CdH_12r") == 0)
1514  CdH_12r = value;
1515  else if (name.compare("CdH_13r") == 0)
1516  CdH_13r = value;
1517  else if (name.compare("CdH_22r") == 0){
1518  if (!FlagFlavU3OfX){
1519  CdH_22r = value;
1520  }
1521  } else if (name.compare("CdH_23r") == 0)
1522  CdH_23r = value;
1523  else if (name.compare("CdH_33r") == 0){
1524  CdH_33r = value;
1525  if (FlagFlavU3OfX){
1526  CdH_11r = value;
1527  CdH_22r = value;
1528  }
1529  } else if (name.compare("CdH_11i") == 0)
1530  CdH_11i = value;
1531  else if (name.compare("CdH_12i") == 0)
1532  CdH_12i = value;
1533  else if (name.compare("CdH_13i") == 0)
1534  CdH_13i = value;
1535  else if (name.compare("CdH_22i") == 0)
1536  CdH_22i = value;
1537  else if (name.compare("CdH_23i") == 0)
1538  CdH_23i = value;
1539  else if (name.compare("CdH_33i") == 0)
1540  CdH_33i = value;
1541  else if (name.compare("CuG_11r") == 0){
1542  if (!FlagFlavU3OfX){
1543  CuG_11r = value;
1544  }
1545  } else if (name.compare("CuG_12r") == 0)
1546  CuG_12r = value;
1547  else if (name.compare("CuG_13r") == 0)
1548  CuG_13r = value;
1549  else if (name.compare("CuG_22r") == 0){
1550  if (!FlagFlavU3OfX){
1551  CuG_22r = value;
1552  }
1553  } else if (name.compare("CuG_23r") == 0)
1554  CuG_23r = value;
1555  else if (name.compare("CuG_33r") == 0){
1556  CuG_33r = value;
1557  if (FlagFlavU3OfX){
1558  CuG_11r = value;
1559  CuG_22r = value;
1560  }
1561  } else if (name.compare("CuG_r") == 0) {
1562  CuG_11r = value;
1563  CuG_12r = 0.0;
1564  CuG_13r = 0.0;
1565  CuG_22r = value;
1566  CuG_23r = 0.0;
1567  CuG_33r = value;
1568  } else if (name.compare("CuG_11i") == 0)
1569  CuG_11i = value;
1570  else if (name.compare("CuG_12i") == 0)
1571  CuG_12i = value;
1572  else if (name.compare("CuG_13i") == 0)
1573  CuG_13i = value;
1574  else if (name.compare("CuG_22i") == 0)
1575  CuG_22i = value;
1576  else if (name.compare("CuG_23i") == 0)
1577  CuG_23i = value;
1578  else if (name.compare("CuG_33i") == 0)
1579  CuG_33i = value;
1580  else if (name.compare("CuG_i") == 0) {
1581  CuG_11i = value;
1582  CuG_12i = 0.0;
1583  CuG_13i = 0.0;
1584  CuG_22i = value;
1585  CuG_23i = 0.0;
1586  CuG_33i = value;
1587  } else if (name.compare("CuW_11r") == 0){
1588  if (!FlagFlavU3OfX){
1589  CuW_11r = value;
1590  }
1591  } else if (name.compare("CuW_12r") == 0)
1592  CuW_12r = value;
1593  else if (name.compare("CuW_13r") == 0)
1594  CuW_13r = value;
1595  else if (name.compare("CuW_22r") == 0){
1596  if (!FlagFlavU3OfX){
1597  CuW_22r = value;
1598  }
1599  } else if (name.compare("CuW_23r") == 0)
1600  CuW_23r = value;
1601  else if (name.compare("CuW_33r") == 0){
1602  CuW_33r = value;
1603  if (FlagFlavU3OfX){
1604  CuW_11r = value;
1605  CuW_22r = value;
1606  }
1607  } else if (name.compare("CuW_r") == 0) {
1608  CuW_11r = value;
1609  CuW_12r = 0.0;
1610  CuW_13r = 0.0;
1611  CuW_22r = value;
1612  CuW_23r = 0.0;
1613  CuW_33r = value;
1614  } else if (name.compare("CuW_11i") == 0)
1615  CuW_11i = value;
1616  else if (name.compare("CuW_12i") == 0)
1617  CuW_12i = value;
1618  else if (name.compare("CuW_13i") == 0)
1619  CuW_13i = value;
1620  else if (name.compare("CuW_22i") == 0)
1621  CuW_22i = value;
1622  else if (name.compare("CuW_23i") == 0)
1623  CuW_23i = value;
1624  else if (name.compare("CuW_33i") == 0)
1625  CuW_33i = value;
1626  else if (name.compare("CuW_i") == 0) {
1627  CuW_11i = value;
1628  CuW_12i = 0.0;
1629  CuW_13i = 0.0;
1630  CuW_22i = value;
1631  CuW_23i = 0.0;
1632  CuW_33i = value;
1633  } else if (name.compare("CuB_11r") == 0){
1634  if (!FlagFlavU3OfX){
1635  CuB_11r = value;
1636  }
1637  } else if (name.compare("CuB_12r") == 0)
1638  CuB_12r = value;
1639  else if (name.compare("CuB_13r") == 0)
1640  CuB_13r = value;
1641  else if (name.compare("CuB_22r") == 0){
1642  if (!FlagFlavU3OfX){
1643  CuB_22r = value;
1644  }
1645  } else if (name.compare("CuB_23r") == 0)
1646  CuB_23r = value;
1647  else if (name.compare("CuB_33r") == 0){
1648  CuB_33r = value;
1649  if (FlagFlavU3OfX){
1650  CuB_11r = value;
1651  CuB_22r = value;
1652  }
1653  } else if (name.compare("CuB_r") == 0) {
1654  CuB_11r = value;
1655  CuB_12r = 0.0;
1656  CuB_13r = 0.0;
1657  CuB_22r = value;
1658  CuB_23r = 0.0;
1659  CuB_33r = value;
1660  } else if (name.compare("CuB_11i") == 0)
1661  CuB_11i = value;
1662  else if (name.compare("CuB_12i") == 0)
1663  CuB_12i = value;
1664  else if (name.compare("CuB_13i") == 0)
1665  CuB_13i = value;
1666  else if (name.compare("CuB_22i") == 0)
1667  CuB_22i = value;
1668  else if (name.compare("CuB_23i") == 0)
1669  CuB_23i = value;
1670  else if (name.compare("CuB_33i") == 0)
1671  CuB_33i = value;
1672  else if (name.compare("CuB_i") == 0) {
1673  CuB_11i = value;
1674  CuB_12i = 0.0;
1675  CuB_13i = 0.0;
1676  CuB_22i = value;
1677  CuB_23i = 0.0;
1678  CuB_33i = value;
1679 // Several redundancies for the 4-fermionn operators below
1680  } else if (name.compare("CLL_1111") == 0) {
1681  CLL_1111 = value;
1682  } else if (name.compare("CLL_1122") == 0) {
1683  CLL_1122 = value;
1684  CLL_2211 = value;
1685  } else if (name.compare("CLL_1133") == 0) {
1686  CLL_1133 = value;
1687  CLL_3311 = value;
1688  } else if (name.compare("CLL_1221") == 0) {
1689  CLL_1221 = value;
1690  CLL_2112 = value;
1691  } else if (name.compare("CLL_1331") == 0) {
1692  CLL_1331 = value;
1693  CLL_3113 = value;
1694  } else if (name.compare("CLL") == 0) {
1695  CLL_1111 = value;
1696  CLL_1221 = value;
1697  CLL_2112 = value;
1698  CLL_2211 = value;
1699  CLL_1122 = value;
1700  CLL_3311 = value;
1701  CLL_1133 = value;
1702  CLL_1331 = value;
1703  CLL_3113 = value;
1704  } else if (name.compare("CLQ1_1111") == 0) {
1705  CLQ1_1111 = value;
1706  } else if (name.compare("CLQ1_1122") == 0) {
1707  CLQ1_1122 = value;
1708  } else if (name.compare("CLQ1_2211") == 0) {
1709  CLQ1_2211 = value;
1710  } else if (name.compare("CLQ1_2112") == 0) {
1711  CLQ1_2112 = value;
1712  } else if (name.compare("CLQ1_1221") == 0) {
1713  CLQ1_1221 = value;
1714  } else if (name.compare("CLQ1_1133") == 0) {
1715  CLQ1_1133 = value;
1716  } else if (name.compare("CLQ1_3311") == 0) {
1717  CLQ1_3311 = value;
1718  } else if (name.compare("CLQ1_3113") == 0) {
1719  CLQ1_3113 = value;
1720  } else if (name.compare("CLQ1_1331") == 0) {
1721  CLQ1_1331 = value;
1722  } else if (name.compare("CLQ1_1123") == 0) {
1723  CLQ1_1123 = value;
1724  } else if (name.compare("CLQ1_2223") == 0) {
1725  CLQ1_2223 = value;
1726  } else if (name.compare("CLQ1_3323") == 0) {
1727  CLQ1_3323 = value;
1728  } else if (name.compare("CLQ1_1132") == 0) {
1729  CLQ1_1132 = value;
1730  } else if (name.compare("CLQ1_2232") == 0) {
1731  CLQ1_2232 = value;
1732  } else if (name.compare("CLQ1_3332") == 0) {
1733  CLQ1_3332 = value;
1734  } else if (name.compare("CLQ1") == 0) {
1735  CLQ1_1111 = value;
1736  CLQ1_1122 = value;
1737  CLQ1_2211 = value;
1738  CLQ1_1221 = value;
1739  CLQ1_2112 = value;
1740  CLQ1_1133 = value;
1741  CLQ1_3311 = value;
1742  CLQ1_1331 = value;
1743  CLQ1_3113 = value;
1744  } else if (name.compare("CLQ3_1111") == 0) {
1745  CLQ3_1111 = value;
1746  } else if (name.compare("CLQ3_1122") == 0) {
1747  CLQ3_1122 = value;
1748  } else if (name.compare("CLQ3_2211") == 0) {
1749  CLQ3_2211 = value;
1750  } else if (name.compare("CLQ3_2112") == 0) {
1751  CLQ3_2112 = value;
1752  } else if (name.compare("CLQ3_1221") == 0) {
1753  CLQ3_1221 = value;
1754  } else if (name.compare("CLQ3_1133") == 0) {
1755  CLQ3_1133 = value;
1756  } else if (name.compare("CLQ3_3311") == 0) {
1757  CLQ3_3311 = value;
1758  } else if (name.compare("CLQ3_3113") == 0) {
1759  CLQ3_3113 = value;
1760  } else if (name.compare("CLQ3_1331") == 0) {
1761  CLQ3_1331 = value;
1762  } else if (name.compare("CLQ3_1123") == 0) {
1763  CLQ3_1123 = value;
1764  } else if (name.compare("CLQ3_2223") == 0) {
1765  CLQ3_2223 = value;
1766  } else if (name.compare("CLQ3_3323") == 0) {
1767  CLQ3_3323 = value;
1768  } else if (name.compare("CLQ3_1132") == 0) {
1769  CLQ3_1132 = value;
1770  } else if (name.compare("CLQ3_2232") == 0) {
1771  CLQ3_2232 = value;
1772  } else if (name.compare("CLQ3_3332") == 0) {
1773  CLQ3_3332 = value;
1774  } else if (name.compare("CLQ3") == 0) {
1775  CLQ3_1111 = value;
1776  CLQ3_1122 = value;
1777  CLQ3_2211 = value;
1778  CLQ3_1221 = value;
1779  CLQ3_2112 = value;
1780  CLQ3_1133 = value;
1781  CLQ3_3311 = value;
1782  CLQ3_1331 = value;
1783  CLQ3_3113 = value;
1784  } else if (name.compare("Cee") == 0) {
1785  Cee_1111 = value;
1786  Cee_1122 = value;
1787  Cee_2211 = value;
1788  Cee_1133 = value;
1789  Cee_3311 = value;
1790  } else if (name.compare("Cee_1111") == 0) {
1791  Cee_1111 = value;
1792  } else if (name.compare("Cee_1122") == 0) {
1793  Cee_1122 = value;
1794  Cee_2211 = value;
1795  } else if (name.compare("Cee_1133") == 0) {
1796  Cee_1133 = value;
1797  Cee_3311 = value;
1798  } else if (name.compare("Ceu") == 0) {
1799  Ceu_1111 = value;
1800  Ceu_1122 = value;
1801  Ceu_2211 = value;
1802  Ceu_1133 = value;
1803  Ceu_2233 = value;
1804  Ceu_3311 = value;
1805  } else if (name.compare("Ceu_1111") == 0) {
1806  Ceu_1111 = value;
1807  } else if (name.compare("Ceu_1122") == 0) {
1808  Ceu_1122 = value;
1809  } else if (name.compare("Ceu_2211") == 0) {
1810  Ceu_2211 = value;
1811  } else if (name.compare("Ceu_1133") == 0) {
1812  Ceu_1133 = value;
1813  } else if (name.compare("Ceu_2233") == 0) {
1814  Ceu_2233 = value;
1815  } else if (name.compare("Ceu_3311") == 0) {
1816  Ceu_3311 = value;
1817  } else if (name.compare("Ced") == 0) {
1818  Ced_1111 = value;
1819  Ced_1122 = value;
1820  Ced_2211 = value;
1821  Ced_1133 = value;
1822  Ced_3311 = value;
1823  } else if (name.compare("Ced_1111") == 0) {
1824  Ced_1111 = value;
1825  } else if (name.compare("Ced_1122") == 0) {
1826  Ced_1122 = value;
1827  } else if (name.compare("Ced_2211") == 0) {
1828  Ced_2211 = value;
1829  } else if (name.compare("Ced_1133") == 0) {
1830  Ced_1133 = value;
1831  } else if (name.compare("Ced_3311") == 0) {
1832  Ced_3311 = value;
1833  } else if (name.compare("Ced_1123") == 0) {
1834  Ced_1123 = value;
1835  } else if (name.compare("Ced_2223") == 0) {
1836  Ced_2223 = value;
1837  } else if (name.compare("Ced_3323") == 0) {
1838  Ced_3323 = value;
1839  } else if (name.compare("Ced_1132") == 0) {
1840  Ced_1132 = value;
1841  } else if (name.compare("Ced_2232") == 0) {
1842  Ced_2232 = value;
1843  } else if (name.compare("Ced_3332") == 0) {
1844  Ced_3332 = value;
1845  } else if (name.compare("CLe") == 0) {
1846  CLe_1111 = value;
1847  CLe_1122 = value;
1848  CLe_2211 = value;
1849  CLe_1133 = value;
1850  CLe_3311 = value;
1851  } else if (name.compare("CLe_1111") == 0) {
1852  CLe_1111 = value;
1853  } else if (name.compare("CLe_1122") == 0) {
1854  CLe_1122 = value;
1855  } else if (name.compare("CLe_2211") == 0) {
1856  CLe_2211 = value;
1857  } else if (name.compare("CLe_1133") == 0) {
1858  CLe_1133 = value;
1859  } else if (name.compare("CLe_3311") == 0) {
1860  CLe_3311 = value;
1861  } else if (name.compare("CLu") == 0) {
1862  CLu_1111 = value;
1863  CLu_1122 = value;
1864  CLu_2211 = value;
1865  CLu_1133 = value;
1866  CLu_2233 = value;
1867  CLu_3311 = value;
1868  } else if (name.compare("CLu_1111") == 0) {
1869  CLu_1111 = value;
1870  } else if (name.compare("CLu_1122") == 0) {
1871  CLu_1122 = value;
1872  } else if (name.compare("CLu_2211") == 0) {
1873  CLu_2211 = value;
1874  } else if (name.compare("CLu_1133") == 0) {
1875  CLu_1133 = value;
1876  } else if (name.compare("CLu_2233") == 0) {
1877  CLu_2233 = value;
1878  } else if (name.compare("CLu_3311") == 0) {
1879  CLu_3311 = value;
1880  } else if (name.compare("CLd") == 0) {
1881  CLd_1111 = value;
1882  CLd_1122 = value;
1883  CLd_2211 = value;
1884  CLd_1133 = value;
1885  CLd_3311 = value;
1886  } else if (name.compare("CLd_1111") == 0) {
1887  CLd_1111 = value;
1888  } else if (name.compare("CLd_1122") == 0) {
1889  CLd_1122 = value;
1890  } else if (name.compare("CLd_2211") == 0) {
1891  CLd_2211 = value;
1892  } else if (name.compare("CLd_1133") == 0) {
1893  CLd_1133 = value;
1894  } else if (name.compare("CLd_3311") == 0) {
1895  CLd_3311 = value;
1896  } else if (name.compare("CLd_1123") == 0) {
1897  CLd_1123 = value;
1898  } else if (name.compare("CLd_2223") == 0) {
1899  CLd_2223 = value;
1900  } else if (name.compare("CLd_3323") == 0) {
1901  CLd_3323 = value;
1902  } else if (name.compare("CLd_1132") == 0) {
1903  CLd_1132 = value;
1904  } else if (name.compare("CLd_2232") == 0) {
1905  CLd_2232 = value;
1906  } else if (name.compare("CLd_3332") == 0) {
1907  CLd_3332 = value;
1908  } else if (name.compare("CQe") == 0) {
1909  CQe_1111 = value;
1910  CQe_1122 = value;
1911  CQe_2211 = value;
1912  CQe_1133 = value;
1913  CQe_3311 = value;
1914  } else if (name.compare("CQe_1111") == 0) {
1915  CQe_1111 = value;
1916  } else if (name.compare("CQe_1122") == 0) {
1917  CQe_1122 = value;
1918  } else if (name.compare("CQe_2211") == 0) {
1919  CQe_2211 = value;
1920  } else if (name.compare("CQe_1133") == 0) {
1921  CQe_1133 = value;
1922  } else if (name.compare("CQe_3311") == 0) {
1923  CQe_3311 = value;
1924  } else if (name.compare("CQe_2311") == 0) {
1925  CQe_2311 = value;
1926  } else if (name.compare("CQe_2322") == 0) {
1927  CQe_2322 = value;
1928  } else if (name.compare("CQe_2333") == 0) {
1929  CQe_2333 = value;
1930  } else if (name.compare("CQe_3211") == 0) {
1931  CQe_3211 = value;
1932  } else if (name.compare("CQe_3222") == 0) {
1933  CQe_3222 = value;
1934  } else if (name.compare("CLedQ_11") == 0) {
1935  CLedQ_11 = value;
1936  } else if (name.compare("CLedQ_22") == 0) {
1937  CLedQ_22 = value;
1938  } else if (name.compare("CpLedQ_11") == 0) {
1939  CpLedQ_11 = value;
1940  } else if (name.compare("CpLedQ_22") == 0) {
1941  CpLedQ_22 = value;
1942  } else if (name.compare("CQe_3233") == 0) {
1943  CQe_3233 = value;
1944  } else if (name.compare("Lambda_NP") == 0) {
1945  Lambda_NP = value;
1946  } else if (name.compare("BrHinv") == 0) {
1947 // Always positive
1948  BrHinv = fabs(value);
1949  } else if (name.compare("BrHexo") == 0) {
1950 // Always positive
1951  BrHexo = fabs(value);
1952  } else if (name.compare("dg1Z") == 0) {
1953  dg1Z = value;
1954  } else if (name.compare("dKappaga") == 0) {
1955  dKappaga = value;
1956  } else if (name.compare("lambZ") == 0) {
1957  lambZ = value;
1958  } else if (name.compare("eggFint") == 0) {
1959  eggFint = value;
1960  } else if (name.compare("eggFpar") == 0) {
1961  eggFpar = value;
1962  } else if (name.compare("ettHint") == 0) {
1963  ettHint = value;
1964  } else if (name.compare("ettHpar") == 0) {
1965  ettHpar = value;
1966  } else if (name.compare("eVBFint") == 0) {
1967  eVBFint = value;
1968  } else if (name.compare("eVBFpar") == 0) {
1969  eVBFpar = value;
1970  } else if (name.compare("eWHint") == 0) {
1971  eWHint = value;
1972  } else if (name.compare("eWHpar") == 0) {
1973  eWHpar = value;
1974  } else if (name.compare("eZHint") == 0) {
1975  eZHint = value;
1976  } else if (name.compare("eZHpar") == 0) {
1977  eZHpar = value;
1978  } else if (name.compare("eeeWBFint") == 0) {
1979  eeeWBFint = value;
1980  } else if (name.compare("eeeWBFpar") == 0) {
1981  eeeWBFpar = value;
1982  } else if (name.compare("eeeZHint") == 0) {
1983  eeeZHint = value;
1984  } else if (name.compare("eeeZHpar") == 0) {
1985  eeeZHpar = value;
1986  } else if (name.compare("eeettHint") == 0) {
1987  eeettHint = value;
1988  } else if (name.compare("eeettHpar") == 0) {
1989  eeettHpar = value;
1990  } else if (name.compare("eepWBFint") == 0) {
1991  eepWBFint = value;
1992  } else if (name.compare("eepWBFpar") == 0) {
1993  eepWBFpar = value;
1994  } else if (name.compare("eepZBFint") == 0) {
1995  eepZBFint = value;
1996  } else if (name.compare("eepZBFpar") == 0) {
1997  eepZBFpar = value;
1998  } else if (name.compare("eHggint") == 0) {
1999  eHggint = value;
2000  } else if (name.compare("eHggpar") == 0) {
2001  eHggpar = value;
2002  } else if (name.compare("eHWWint") == 0) {
2003  eHWWint = value;
2004  } else if (name.compare("eHWWpar") == 0) {
2005  eHWWpar = value;
2006  } else if (name.compare("eHZZint") == 0) {
2007  eHZZint = value;
2008  } else if (name.compare("eHZZpar") == 0) {
2009  eHZZpar = value;
2010  } else if (name.compare("eHZgaint") == 0) {
2011  eHZgaint = value;
2012  } else if (name.compare("eHZgapar") == 0) {
2013  eHZgapar = value;
2014  } else if (name.compare("eHgagaint") == 0) {
2015  eHgagaint = value;
2016  } else if (name.compare("eHgagapar") == 0) {
2017  eHgagapar = value;
2018  } else if (name.compare("eHmumuint") == 0) {
2019  eHmumuint = value;
2020  } else if (name.compare("eHmumupar") == 0) {
2021  eHmumupar = value;
2022  } else if (name.compare("eHtautauint") == 0) {
2023  eHtautauint = value;
2024  } else if (name.compare("eHtautaupar") == 0) {
2025  eHtautaupar = value;
2026  } else if (name.compare("eHccint") == 0) {
2027  eHccint = value;
2028  } else if (name.compare("eHccpar") == 0) {
2029  eHccpar = value;
2030  } else if (name.compare("eHbbint") == 0) {
2031  eHbbint = value;
2032  } else if (name.compare("eHbbpar") == 0) {
2033  eHbbpar = value;
2034  } else if (name.compare("eggFHgaga") == 0) {
2035  eggFHgaga = value;
2036  } else if (name.compare("eggFHZga") == 0) {
2037  eggFHZga = value;
2038  } else if (name.compare("eggFHZZ") == 0) {
2039  eggFHZZ = value;
2040  } else if (name.compare("eggFHWW") == 0) {
2041  eggFHWW = value;
2042  } else if (name.compare("eggFHtautau") == 0) {
2043  eggFHtautau = value;
2044  } else if (name.compare("eggFHbb") == 0) {
2045  eggFHbb = value;
2046  } else if (name.compare("eggFHmumu") == 0) {
2047  eggFHmumu = value;
2048  } else if (name.compare("eVBFHgaga") == 0) {
2049  eVBFHgaga = value;
2050  } else if (name.compare("eVBFHZga") == 0) {
2051  eVBFHZga = value;
2052  } else if (name.compare("eVBFHZZ") == 0) {
2053  eVBFHZZ = value;
2054  } else if (name.compare("eVBFHWW") == 0) {
2055  eVBFHWW = value;
2056  } else if (name.compare("eVBFHtautau") == 0) {
2057  eVBFHtautau = value;
2058  } else if (name.compare("eVBFHbb") == 0) {
2059  eVBFHbb = value;
2060  } else if (name.compare("eVBFHmumu") == 0) {
2061  eVBFHmumu = value;
2062  } else if (name.compare("eWHgaga") == 0) {
2063  eWHgaga = value;
2064  } else if (name.compare("eWHZga") == 0) {
2065  eWHZga = value;
2066  } else if (name.compare("eWHZZ") == 0) {
2067  eWHZZ = value;
2068  } else if (name.compare("eWHWW") == 0) {
2069  eWHWW = value;
2070  } else if (name.compare("eWHtautau") == 0) {
2071  eWHtautau = value;
2072  } else if (name.compare("eWHbb") == 0) {
2073  eWHbb = value;
2074  } else if (name.compare("eWHmumu") == 0) {
2075  eWHmumu = value;
2076  } else if (name.compare("eZHgaga") == 0) {
2077  eZHgaga = value;
2078  } else if (name.compare("eZHZga") == 0) {
2079  eZHZga = value;
2080  } else if (name.compare("eZHZZ") == 0) {
2081  eZHZZ = value;
2082  } else if (name.compare("eZHWW") == 0) {
2083  eZHWW = value;
2084  } else if (name.compare("eZHtautau") == 0) {
2085  eZHtautau = value;
2086  } else if (name.compare("eZHbb") == 0) {
2087  eZHbb = value;
2088  } else if (name.compare("eZHmumu") == 0) {
2089  eZHmumu = value;
2090  } else if (name.compare("ettHgaga") == 0) {
2091  ettHgaga = value;
2092  } else if (name.compare("ettHZga") == 0) {
2093  ettHZga = value;
2094  } else if (name.compare("ettHZZ") == 0) {
2095  ettHZZ = value;
2096  } else if (name.compare("ettHWW") == 0) {
2097  ettHWW = value;
2098  } else if (name.compare("ettHtautau") == 0) {
2099  ettHtautau = value;
2100  } else if (name.compare("ettHbb") == 0) {
2101  ettHbb = value;
2102  } else if (name.compare("ettHmumu") == 0) {
2103  ettHmumu = value;
2104  } else if (name.compare("eVBFHinv") == 0) {
2105  eVBFHinv = value;
2106  } else if (name.compare("eVHinv") == 0) {
2107  eVHinv = value;
2108  } else if (name.compare("eVBF_2_Hbox") == 0) {
2109  eVBF_2_Hbox = value;
2110  } else if (name.compare("eVBF_2_HQ1_11") == 0) {
2111  eVBF_2_HQ1_11 = value;
2112  } else if (name.compare("eVBF_2_Hu_11") == 0) {
2113  eVBF_2_Hu_11 = value;
2114  } else if (name.compare("eVBF_2_Hd_11") == 0) {
2115  eVBF_2_Hd_11 = value;
2116  } else if (name.compare("eVBF_2_HQ3_11") == 0) {
2117  eVBF_2_HQ3_11 = value;
2118  } else if (name.compare("eVBF_2_HD") == 0) {
2119  eVBF_2_HD = value;
2120  } else if (name.compare("eVBF_2_HB") == 0) {
2121  eVBF_2_HB = value;
2122  } else if (name.compare("eVBF_2_HW") == 0) {
2123  eVBF_2_HW = value;
2124  } else if (name.compare("eVBF_2_HWB") == 0) {
2125  eVBF_2_HWB = value;
2126  } else if (name.compare("eVBF_2_HG") == 0) {
2127  eVBF_2_HG = value;
2128  } else if (name.compare("eVBF_2_DHB") == 0) {
2129  eVBF_2_DHB = value;
2130  } else if (name.compare("eVBF_2_DHW") == 0) {
2131  eVBF_2_DHW = value;
2132  } else if (name.compare("eVBF_2_DeltaGF") == 0) {
2133  eVBF_2_DeltaGF = value;
2134  } else if (name.compare("eVBF_78_Hbox") == 0) {
2135  eVBF_78_Hbox = value;
2136  } else if (name.compare("eVBF_78_HQ1_11") == 0) {
2137  eVBF_78_HQ1_11 = value;
2138  } else if (name.compare("eVBF_78_Hu_11") == 0) {
2139  eVBF_78_Hu_11 = value;
2140  } else if (name.compare("eVBF_78_Hd_11") == 0) {
2141  eVBF_78_Hd_11 = value;
2142  } else if (name.compare("eVBF_78_HQ3_11") == 0) {
2143  eVBF_78_HQ3_11 = value;
2144  } else if (name.compare("eVBF_78_HD") == 0) {
2145  eVBF_78_HD = value;
2146  } else if (name.compare("eVBF_78_HB") == 0) {
2147  eVBF_78_HB = value;
2148  } else if (name.compare("eVBF_78_HW") == 0) {
2149  eVBF_78_HW = value;
2150  } else if (name.compare("eVBF_78_HWB") == 0) {
2151  eVBF_78_HWB = value;
2152  } else if (name.compare("eVBF_78_HG") == 0) {
2153  eVBF_78_HG = value;
2154  } else if (name.compare("eVBF_78_DHB") == 0) {
2155  eVBF_78_DHB = value;
2156  } else if (name.compare("eVBF_78_DHW") == 0) {
2157  eVBF_78_DHW = value;
2158  } else if (name.compare("eVBF_78_DeltaGF") == 0) {
2159  eVBF_78_DeltaGF = value;
2160  } else if (name.compare("eVBF_1314_Hbox") == 0) {
2161  eVBF_1314_Hbox = value;
2162  } else if (name.compare("eVBF_1314_HQ1_11") == 0) {
2163  eVBF_1314_HQ1_11 = value;
2164  } else if (name.compare("eVBF_1314_Hu_11") == 0) {
2165  eVBF_1314_Hu_11 = value;
2166  } else if (name.compare("eVBF_1314_Hd_11") == 0) {
2167  eVBF_1314_Hd_11 = value;
2168  } else if (name.compare("eVBF_1314_HQ3_11") == 0) {
2169  eVBF_1314_HQ3_11 = value;
2170  } else if (name.compare("eVBF_1314_HD") == 0) {
2171  eVBF_1314_HD = value;
2172  } else if (name.compare("eVBF_1314_HB") == 0) {
2173  eVBF_1314_HB = value;
2174  } else if (name.compare("eVBF_1314_HW") == 0) {
2175  eVBF_1314_HW = value;
2176  } else if (name.compare("eVBF_1314_HWB") == 0) {
2177  eVBF_1314_HWB = value;
2178  } else if (name.compare("eVBF_1314_HG") == 0) {
2179  eVBF_1314_HG = value;
2180  } else if (name.compare("eVBF_1314_DHB") == 0) {
2181  eVBF_1314_DHB = value;
2182  } else if (name.compare("eVBF_1314_DHW") == 0) {
2183  eVBF_1314_DHW = value;
2184  } else if (name.compare("eVBF_1314_DeltaGF") == 0) {
2185  eVBF_1314_DeltaGF = value;
2186  } else if (name.compare("eWH_2_Hbox") == 0) {
2187  eWH_2_Hbox = value;
2188  } else if (name.compare("eWH_2_HQ3_11") == 0) {
2189  eWH_2_HQ3_11 = value;
2190  } else if (name.compare("eWH_2_HD") == 0) {
2191  eWH_2_HD = value;
2192  } else if (name.compare("eWH_2_HW") == 0) {
2193  eWH_2_HW = value;
2194  } else if (name.compare("eWH_2_HWB") == 0) {
2195  eWH_2_HWB = value;
2196  } else if (name.compare("eWH_2_DHW") == 0) {
2197  eWH_2_DHW = value;
2198  } else if (name.compare("eWH_2_DeltaGF") == 0) {
2199  eWH_2_DeltaGF = value;
2200  } else if (name.compare("eWH_78_Hbox") == 0) {
2201  eWH_78_Hbox = value;
2202  } else if (name.compare("eWH_78_HQ3_11") == 0) {
2203  eWH_78_HQ3_11 = value;
2204  } else if (name.compare("eWH_78_HD") == 0) {
2205  eWH_78_HD = value;
2206  } else if (name.compare("eWH_78_HW") == 0) {
2207  eWH_78_HW = value;
2208  } else if (name.compare("eWH_78_HWB") == 0) {
2209  eWH_78_HWB = value;
2210  } else if (name.compare("eWH_78_DHW") == 0) {
2211  eWH_78_DHW = value;
2212  } else if (name.compare("eWH_78_DeltaGF") == 0) {
2213  eWH_78_DeltaGF = value;
2214  } else if (name.compare("eWH_1314_Hbox") == 0) {
2215  eWH_1314_Hbox = value;
2216  } else if (name.compare("eWH_1314_HQ3_11") == 0) {
2217  eWH_1314_HQ3_11 = value;
2218  } else if (name.compare("eWH_1314_HD") == 0) {
2219  eWH_1314_HD = value;
2220  } else if (name.compare("eWH_1314_HW") == 0) {
2221  eWH_1314_HW = value;
2222  } else if (name.compare("eWH_1314_HWB") == 0) {
2223  eWH_1314_HWB = value;
2224  } else if (name.compare("eWH_1314_DHW") == 0) {
2225  eWH_1314_DHW = value;
2226  } else if (name.compare("eWH_1314_DeltaGF") == 0) {
2227  eWH_1314_DeltaGF = value;
2228  } else if (name.compare("eZH_2_Hbox") == 0) {
2229  eZH_2_Hbox = value;
2230  } else if (name.compare("eZH_2_HQ1_11") == 0) {
2231  eZH_2_HQ1_11 = value;
2232  } else if (name.compare("eZH_2_Hu_11") == 0) {
2233  eZH_2_Hu_11 = value;
2234  } else if (name.compare("eZH_2_Hd_11") == 0) {
2235  eZH_2_Hd_11 = value;
2236  } else if (name.compare("eZH_2_HQ3_11") == 0) {
2237  eZH_2_HQ3_11 = value;
2238  } else if (name.compare("eZH_2_HD") == 0) {
2239  eZH_2_HD = value;
2240  } else if (name.compare("eZH_2_HB") == 0) {
2241  eZH_2_HB = value;
2242  } else if (name.compare("eZH_2_HW") == 0) {
2243  eZH_2_HW = value;
2244  } else if (name.compare("eZH_2_HWB") == 0) {
2245  eZH_2_HWB = value;
2246  } else if (name.compare("eZH_2_DHB") == 0) {
2247  eZH_2_DHB = value;
2248  } else if (name.compare("eZH_2_DHW") == 0) {
2249  eZH_2_DHW = value;
2250  } else if (name.compare("eZH_2_DeltaGF") == 0) {
2251  eZH_2_DeltaGF = value;
2252  } else if (name.compare("eZH_78_Hbox") == 0) {
2253  eZH_78_Hbox = value;
2254  } else if (name.compare("eZH_78_HQ1_11") == 0) {
2255  eZH_78_HQ1_11 = value;
2256  } else if (name.compare("eZH_78_Hu_11") == 0) {
2257  eZH_78_Hu_11 = value;
2258  } else if (name.compare("eZH_78_Hd_11") == 0) {
2259  eZH_78_Hd_11 = value;
2260  } else if (name.compare("eZH_78_HQ3_11") == 0) {
2261  eZH_78_HQ3_11 = value;
2262  } else if (name.compare("eZH_78_HD") == 0) {
2263  eZH_78_HD = value;
2264  } else if (name.compare("eZH_78_HB") == 0) {
2265  eZH_78_HB = value;
2266  } else if (name.compare("eZH_78_HW") == 0) {
2267  eZH_78_HW = value;
2268  } else if (name.compare("eZH_78_HWB") == 0) {
2269  eZH_78_HWB = value;
2270  } else if (name.compare("eZH_78_DHB") == 0) {
2271  eZH_78_DHB = value;
2272  } else if (name.compare("eZH_78_DHW") == 0) {
2273  eZH_78_DHW = value;
2274  } else if (name.compare("eZH_78_DeltaGF") == 0) {
2275  eZH_78_DeltaGF = value;
2276  } else if (name.compare("eZH_1314_Hbox") == 0) {
2277  eZH_1314_Hbox = value;
2278  } else if (name.compare("eZH_1314_HQ1_11") == 0) {
2279  eZH_1314_HQ1_11 = value;
2280  } else if (name.compare("eZH_1314_Hu_11") == 0) {
2281  eZH_1314_Hu_11 = value;
2282  } else if (name.compare("eZH_1314_Hd_11") == 0) {
2283  eZH_1314_Hd_11 = value;
2284  } else if (name.compare("eZH_1314_HQ3_11") == 0) {
2285  eZH_1314_HQ3_11 = value;
2286  } else if (name.compare("eZH_1314_HD") == 0) {
2287  eZH_1314_HD = value;
2288  } else if (name.compare("eZH_1314_HB") == 0) {
2289  eZH_1314_HB = value;
2290  } else if (name.compare("eZH_1314_HW") == 0) {
2291  eZH_1314_HW = value;
2292  } else if (name.compare("eZH_1314_HWB") == 0) {
2293  eZH_1314_HWB = value;
2294  } else if (name.compare("eZH_1314_DHB") == 0) {
2295  eZH_1314_DHB = value;
2296  } else if (name.compare("eZH_1314_DHW") == 0) {
2297  eZH_1314_DHW = value;
2298  } else if (name.compare("eZH_1314_DeltaGF") == 0) {
2299  eZH_1314_DeltaGF = value;
2300  } else if (name.compare("ettH_2_HG") == 0) {
2301  ettH_2_HG = value;
2302  } else if (name.compare("ettH_2_G") == 0) {
2303  ettH_2_G = value;
2304  } else if (name.compare("ettH_2_uG_33r") == 0) {
2305  ettH_2_uG_33r = value;
2306  } else if (name.compare("ettH_2_DeltagHt") == 0) {
2307  ettH_2_DeltagHt = value;
2308  } else if (name.compare("ettH_78_HG") == 0) {
2309  ettH_78_HG = value;
2310  } else if (name.compare("ettH_78_G") == 0) {
2311  ettH_78_G = value;
2312  } else if (name.compare("ettH_78_uG_33r") == 0) {
2313  ettH_78_uG_33r = value;
2314  } else if (name.compare("ettH_78_DeltagHt") == 0) {
2315  ettH_78_DeltagHt = value;
2316  } else if (name.compare("ettH_1314_HG") == 0) {
2317  ettH_1314_HG = value;
2318  } else if (name.compare("ettH_1314_G") == 0) {
2319  ettH_1314_G = value;
2320  } else if (name.compare("ettH_1314_uG_33r") == 0) {
2321  ettH_1314_uG_33r = value;
2322  } else if (name.compare("ettH_1314_DeltagHt") == 0) {
2323  ettH_1314_DeltagHt = value;
2324  } else
2325  NPbase::setParameter(name, value);
2326 }

◆ STXS_ggH0j()

double NPSMEFTd6::STXS_ggH0j ( const double  sqrt_s) const
virtual

The STXS bin \(gg \to H\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 14734 of file NPSMEFTd6.cpp.

14734  {
14735 
14736  double STXSb = 1.0;
14737 
14738  STXSb = 1.0 + 55.2*aiG + 0.362*ai3G + 0.276*ai2G;
14739 
14740  return STXSb;
14741 }

◆ STXS_ggH1j_pTH_0_60()

double NPSMEFTd6::STXS_ggH1j_pTH_0_60 ( const double  sqrt_s) const
virtual

The STXS bin \(gg \to H\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 14744 of file NPSMEFTd6.cpp.

14744  {
14745 
14746  double STXSb = 1.0;
14747 
14748  STXSb = 1.0 + 56.0*aiG + 1.52*ai3G + 1.19*ai2G;
14749 
14750  return STXSb;
14751 }

◆ STXS_ggH1j_pTH_120_200()

double NPSMEFTd6::STXS_ggH1j_pTH_120_200 ( const double  sqrt_s) const
virtual

The STXS bin \(gg \to H\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 14764 of file NPSMEFTd6.cpp.

14764  {
14765 
14766  double STXSb = 1.0;
14767 
14768  STXSb = 1.0 + 56.5*aiG + 17.8*ai3G + 11.2*ai2G;
14769 
14770  return STXSb;
14771 }

◆ STXS_ggH1j_pTH_200()

double NPSMEFTd6::STXS_ggH1j_pTH_200 ( const double  sqrt_s) const
virtual

The STXS bin \(gg \to H\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 14774 of file NPSMEFTd6.cpp.

14774  {
14775 
14776  double STXSb = 1.0;
14777 
14778  STXSb = 1.0 + 55.0*aiG + 52.0*ai3G + 34.0*ai2G;
14779 
14780  return STXSb;
14781 }

◆ STXS_ggH1j_pTH_60_120()

double NPSMEFTd6::STXS_ggH1j_pTH_60_120 ( const double  sqrt_s) const
virtual

The STXS bin \(gg \to H\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 14754 of file NPSMEFTd6.cpp.

14754  {
14755 
14756  double STXSb = 1.0;
14757 
14758  STXSb = 1.0 + 55.5*aiG + 4.12*ai3G + 2.76*ai2G;
14759 
14760  return STXSb;
14761 }

◆ STXS_ggH2j_pTH_0_200()

double NPSMEFTd6::STXS_ggH2j_pTH_0_200 ( const double  sqrt_s) const
virtual

The STXS bin \(gg \to H\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 14784 of file NPSMEFTd6.cpp.

14784  {
14785 
14786  double STXSb = 1.0;
14787 
14788  return STXSb;
14789 }

◆ STXS_ggH2j_pTH_0_60()

double NPSMEFTd6::STXS_ggH2j_pTH_0_60 ( const double  sqrt_s) const
virtual

The STXS bin \(gg \to H\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 14792 of file NPSMEFTd6.cpp.

14792  {
14793 
14794  double STXSb = 1.0;
14795 
14796  STXSb = 1.0 + 55.6*aiG + 3.66*ai3G + 4.23*ai2G;
14797 
14798  return STXSb;
14799 }

◆ STXS_ggH2j_pTH_120_200()

double NPSMEFTd6::STXS_ggH2j_pTH_120_200 ( const double  sqrt_s) const
virtual

The STXS bin \(gg \to H\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 14810 of file NPSMEFTd6.cpp.

14810  {
14811 
14812  double STXSb = 1.0;
14813 
14814  STXSb = 1.0 + 55.8*aiG + 23.0*ai3G + 17.5*ai2G;
14815 
14816  return STXSb;
14817 }

◆ STXS_ggH2j_pTH_200()

double NPSMEFTd6::STXS_ggH2j_pTH_200 ( const double  sqrt_s) const
virtual

The STXS bin \(gg \to H\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 14819 of file NPSMEFTd6.cpp.

14819  {
14820 
14821  double STXSb = 1.0;
14822 
14823  STXSb = 1.0 + 56.0*aiG + 89.8*ai3G + 68.1*ai2G;
14824 
14825  return STXSb;
14826 }

◆ STXS_ggH2j_pTH_60_120()

double NPSMEFTd6::STXS_ggH2j_pTH_60_120 ( const double  sqrt_s) const
virtual

The STXS bin \(gg \to H\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 14801 of file NPSMEFTd6.cpp.

14801  {
14802 
14803  double STXSb = 1.0;
14804 
14805  STXSb = 1.0 + 56.1*aiG + 7.73*ai3G + 6.81*ai2G;
14806 
14807  return STXSb;
14808 }

◆ STXS_ggH_VBFtopo_j3()

double NPSMEFTd6::STXS_ggH_VBFtopo_j3 ( const double  sqrt_s) const
virtual

The STXS bin \(gg \to H\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 14724 of file NPSMEFTd6.cpp.

14724  {
14725 
14726  double STXSb = 1.0;
14727 
14728  STXSb = 1.0 + 55.9*aiG + 9.04*ai3G + 8.1*ai2G;
14729 
14730  return STXSb;
14731 }

◆ STXS_ggH_VBFtopo_j3v()

double NPSMEFTd6::STXS_ggH_VBFtopo_j3v ( const double  sqrt_s) const
virtual

The STXS bin \(gg \to H\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 14715 of file NPSMEFTd6.cpp.

14715  {
14716 
14717  double STXSb = 1.0;
14718 
14719  STXSb = 1.0 + 56.6*aiG + 5.5*ai3G + 4.36*ai2G;
14720 
14721  return STXSb;
14722 }

◆ STXS_qqHll_pTV_0_150()

double NPSMEFTd6::STXS_qqHll_pTV_0_150 ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H \ell \ell\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 14932 of file NPSMEFTd6.cpp.

14932  {
14933 
14934  double STXSb = 1.0;
14935 
14936  STXSb = 1.0 - 1.0*aiH - 4.001*aiT + 29.82*aiWW + 8.43*aiB + 8.5*aiHW
14937  + 2.545*aiHB + 0.0315*aiA - 1.89*aiHQ + 22.84*aipHQ + 5.247*aiHu
14938  - 2.0*aiHd - 0.963*aiHL + 2.042*aipHL - 0.2307*aiHe;
14939 
14940  return STXSb;
14941 }

◆ STXS_qqHll_pTV_150_250()

double NPSMEFTd6::STXS_qqHll_pTV_150_250 ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H \ell \ell\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 14944 of file NPSMEFTd6.cpp.

14944  {
14945 
14946  double STXSb = 1.0;
14947 
14948  return STXSb;
14949 }

◆ STXS_qqHll_pTV_150_250_0j()

double NPSMEFTd6::STXS_qqHll_pTV_150_250_0j ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H \ell \ell\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 14952 of file NPSMEFTd6.cpp.

14952  {
14953 
14954  double STXSb = 1.0;
14955 
14956  STXSb = 1.0 - 0.993*aiH - 4.0*aiT + 62.4*aiWW + 18.08*aiB + 37.6*aiHW
14957  + 11.22*aiHB - 5.03*aiHQ + 61.0*aipHQ + 14.39*aiHu - 5.17*aiHd
14958  - 0.977*aiHL + 2.08*aipHL - 0.234*aiHe;
14959 
14960  return STXSb;
14961 }

◆ STXS_qqHll_pTV_150_250_1j()

double NPSMEFTd6::STXS_qqHll_pTV_150_250_1j ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H \ell \ell\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 14964 of file NPSMEFTd6.cpp.

14964  {
14965 
14966  double STXSb = 1.0;
14967 
14968  STXSb = 1.0 - 1.002*aiH - 4.01*aiT + 57.9*aiWW + 16.78*aiB + 32.8*aiHW
14969  + 9.86*aiHB - 4.58*aiHQ + 55.6*aipHQ + 13.54*aiHu - 4.56*aiHd
14970  - 0.989*aiHL + 2.09*aipHL - 0.235*aiHe;
14971 
14972  return STXSb;
14973 }

◆ STXS_qqHll_pTV_250()

double NPSMEFTd6::STXS_qqHll_pTV_250 ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H \ell \ell\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 14976 of file NPSMEFTd6.cpp.

14976  {
14977 
14978  double STXSb = 1.0;
14979 
14980  STXSb = 1.0 - 0.998*aiH - 4.0*aiT + 153.1*aiWW + 45.6*aiB + 126.4*aiHW
14981  + 37.9*aiHB - 13.85*aiHQ + 168.6*aipHQ + 41.7*aiHu - 13.48*aiHd
14982  - 0.977*aiHL + 2.09*aipHL - 0.238*aiHe;
14983 
14984  return STXSb;
14985 }

◆ STXS_qqHlv_pTV_0_150()

double NPSMEFTd6::STXS_qqHlv_pTV_0_150 ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H \ell \nu\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 14892 of file NPSMEFTd6.cpp.

14892  {
14893 
14894  double STXSb = 1.0;
14895 
14896  STXSb = 1.0 - 1.001*aiH + 33.63*aiWW + 11.49*aiHW + 23.62*aipHQ + 2.013*aipHL;
14897 
14898  return STXSb;
14899 }

◆ STXS_qqHlv_pTV_0_250()

double NPSMEFTd6::STXS_qqHlv_pTV_0_250 ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H \ell \nu\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 14884 of file NPSMEFTd6.cpp.

14884  {
14885 
14886  double STXSb = 1.0;
14887 
14888  return STXSb;
14889 }

◆ STXS_qqHlv_pTV_150_250_0j()

double NPSMEFTd6::STXS_qqHlv_pTV_150_250_0j ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H \ell \nu\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 14902 of file NPSMEFTd6.cpp.

14902  {
14903 
14904  double STXSb = 1.0;
14905 
14906  STXSb = 1.0 - 0.998*aiH + 76.3*aiWW + 50.7*aiHW + 66.5*aipHQ + 2.03*aipHL;
14907 
14908  return STXSb;
14909 }

◆ STXS_qqHlv_pTV_150_250_1j()

double NPSMEFTd6::STXS_qqHlv_pTV_150_250_1j ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H \ell \nu\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 14912 of file NPSMEFTd6.cpp.

14912  {
14913 
14914  double STXSb = 1.0;
14915 
14916  STXSb = 1.0 - 1.006*aiH + 70.9*aiWW + 45.5*aiHW + 60.8*aipHQ + 2.04*aipHL;
14917 
14918  return STXSb;
14919 }

◆ STXS_qqHlv_pTV_250()

double NPSMEFTd6::STXS_qqHlv_pTV_250 ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H \ell \nu\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 14922 of file NPSMEFTd6.cpp.

14922  {
14923 
14924  double STXSb = 1.0;
14925 
14926  STXSb = 1.0 - 1.001*aiH + 196.5*aiWW + 169.4*aiHW + 186.3*aipHQ + 2.03*aipHL;
14927 
14928  return STXSb;
14929 }

◆ STXS_qqHqq_pTj_200()

double NPSMEFTd6::STXS_qqHqq_pTj_200 ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H qq\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 14874 of file NPSMEFTd6.cpp.

14874  {
14875 
14876  double STXSb = 1.0;
14877 
14878  STXSb = 1.0 + 7.82*aiWW - 0.1868*aiB - 30.65*aiHW - 2.371*aiHB;
14879 
14880  return STXSb;
14881 }

◆ STXS_qqHqq_Rest()

double NPSMEFTd6::STXS_qqHqq_Rest ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H qq\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 14864 of file NPSMEFTd6.cpp.

14864  {
14865 
14866  double STXSb = 1.0;
14867 
14868  STXSb = 1.0 + 1.546*aiWW - 0.02509*aiB - 3.631*aiHW - 0.2361*aiHB;
14869 
14870  return STXSb;
14871 }

◆ STXS_qqHqq_VBFtopo_j3()

double NPSMEFTd6::STXS_qqHqq_VBFtopo_j3 ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H qq\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 14844 of file NPSMEFTd6.cpp.

14844  {
14845 
14846  double STXSb = 1.0;
14847 
14848  STXSb = 1.0 + 1.204*aiWW - 0.02692*aiB - 5.76*aiHW - 0.4058*aiHB;
14849 
14850  return STXSb;
14851 }

◆ STXS_qqHqq_VBFtopo_j3v()

double NPSMEFTd6::STXS_qqHqq_VBFtopo_j3v ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H qq\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 14835 of file NPSMEFTd6.cpp.

14835  {
14836 
14837  double STXSb = 1.0;
14838 
14839  STXSb = 1.0 + 1.256*aiWW - 0.02319*aiB - 4.31*aiHW - 0.2907*aiHB;
14840 
14841  return STXSb;
14842 }

◆ STXS_qqHqq_VBFtopo_Rest()

double NPSMEFTd6::STXS_qqHqq_VBFtopo_Rest ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H qq\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 14829 of file NPSMEFTd6.cpp.

14829  {
14830 
14831  return STXS_qqHqq_Rest(sqrt_s);
14832 }

◆ STXS_qqHqq_VHtopo()

double NPSMEFTd6::STXS_qqHqq_VHtopo ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H qq\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 14854 of file NPSMEFTd6.cpp.

14854  {
14855 
14856  double STXSb = 1.0;
14857 
14858  STXSb = 1.0 + 1.389*aiWW - 0.0284*aiB - 6.23*aiHW - 0.417*aiHB;
14859 
14860  return STXSb;
14861 }

◆ STXS_ttHtH()

double NPSMEFTd6::STXS_ttHtH ( const double  sqrt_s) const
virtual

The STXS bin \( ttH + tH \).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 14988 of file NPSMEFTd6.cpp.

14988  {
14989 
14990  double STXSb = 1.0;
14991 
14992  STXSb = 1.0 - 0.983*aiH + 2.949*aiu + 0.928*aiG + 313.6*aiuG
14993  + 27.48*ai3G - 13.09*ai2G;
14994 
14995  return STXSb;
14996 }

◆ STXS_WHqqHqq_pTj1_200()

double NPSMEFTd6::STXS_WHqqHqq_pTj1_200 ( const double  sqrt_s) const
virtual

The STXS bin \( qq \to WH \to H qq \).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15034 of file NPSMEFTd6.cpp.

15034  {
15035 
15036  double STXSb = 1.0;
15037 
15038  STXSb = 1.0 - 1.003*aiH + 181.2*aiWW + 152.3*aiHW + 173.7*aipHQ;
15039 
15040  return STXSb;
15041 }

◆ STXS_WHqqHqq_Rest()

double NPSMEFTd6::STXS_WHqqHqq_Rest ( const double  sqrt_s) const
virtual

The STXS bin \( qq \to WH \to H qq \).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15025 of file NPSMEFTd6.cpp.

15025  {
15026 
15027  double STXSb = 1.0;
15028 
15029  STXSb = 1.0 - 1.002*aiH + 34.29*aiWW + 11.56*aiHW + 26.27*aipHQ;
15030 
15031  return STXSb;
15032 }

◆ STXS_WHqqHqq_VBFtopo_j3()

double NPSMEFTd6::STXS_WHqqHqq_VBFtopo_j3 ( const double  sqrt_s) const
virtual

The STXS bin \( qq \to WH \to H qq \).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15007 of file NPSMEFTd6.cpp.

15007  {
15008 
15009  double STXSb = 1.0;
15010 
15011  STXSb = 1.0 - 1.04*aiH + 44.9*aiWW + 20.3*aiHW + 36.8*aipHQ;
15012 
15013  return STXSb;
15014 }

◆ STXS_WHqqHqq_VBFtopo_j3v()

double NPSMEFTd6::STXS_WHqqHqq_VBFtopo_j3v ( const double  sqrt_s) const
virtual

The STXS bin \( qq \to WH \to H qq \).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 14998 of file NPSMEFTd6.cpp.

14998  {
14999 
15000  double STXSb = 1.0;
15001 
15002  STXSb = 1.0 - 0.94*aiH + 39.5*aiWW + 13.8*aiHW + 32.1*aipHQ;
15003 
15004  return STXSb;
15005 }

◆ STXS_WHqqHqq_VH2j()

double NPSMEFTd6::STXS_WHqqHqq_VH2j ( const double  sqrt_s) const
virtual

The STXS bin \( qq \to WH \to H qq \).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15016 of file NPSMEFTd6.cpp.

15016  {
15017 
15018  double STXSb = 1.0;
15019 
15020  STXSb = 1.0 - 0.996*aiH + 45.57*aiWW + 23.66*aiHW + 37.55*aipHQ;
15021 
15022  return STXSb;
15023 }

◆ STXS_ZHqqHqq_pTj1_200()

double NPSMEFTd6::STXS_ZHqqHqq_pTj1_200 ( const double  sqrt_s) const
virtual

The STXS bin \( qq \to ZH \to H qq \).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15083 of file NPSMEFTd6.cpp.

15083  {
15084 
15085  double STXSb = 1.0;
15086 
15087  STXSb = 1.0 - 1.003*aiH - 4.03*aiT + 141.5*aiWW + 41.6*aiB + 112.5*aiHW
15088  + 33.6*aiHB - 11.52*aiHQ + 156.2*aipHQ + 38.9*aiHu - 12.53*aiHd;
15089 
15090  return STXSb;
15091 }

◆ STXS_ZHqqHqq_Rest()

double NPSMEFTd6::STXS_ZHqqHqq_Rest ( const double  sqrt_s) const
virtual

The STXS bin \( qq \to ZH \to H qq \).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15073 of file NPSMEFTd6.cpp.

15073  {
15074 
15075  double STXSb = 1.0;
15076 
15077  STXSb = 1.0 - 1.001*aiH - 3.998*aiT + 30.89*aiWW + 8.35*aiB + 8.71*aiHW
15078  + 2.616*aiHB - 1.782*aiHQ + 26.1*aipHQ + 5.942*aiHu - 2.305*aiHd;
15079 
15080  return STXSb;
15081 }

◆ STXS_ZHqqHqq_VBFtopo_j3()

double NPSMEFTd6::STXS_ZHqqHqq_VBFtopo_j3 ( const double  sqrt_s) const
virtual

The STXS bin \( qq \to ZH \to H qq \).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15053 of file NPSMEFTd6.cpp.

15053  {
15054 
15055  double STXSb = 1.0;
15056 
15057  STXSb = 1.0 - 0.97*aiH - 3.98*aiT + 38.1*aiWW + 10.5*aiB + 14.2*aiHW
15058  + 4.15*aiHB - 2.36*aiHQ + 34.5*aipHQ + 8.4*aiHu - 2.79*aiHd;
15059 
15060  return STXSb;
15061 }

◆ STXS_ZHqqHqq_VBFtopo_j3v()

double NPSMEFTd6::STXS_ZHqqHqq_VBFtopo_j3v ( const double  sqrt_s) const
virtual

The STXS bin \( qq \to ZH \to H qq \).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15043 of file NPSMEFTd6.cpp.

15043  {
15044 
15045  double STXSb = 1.0;
15046 
15047  STXSb = 1.0 - 0.94*aiH - 4.0*aiT + 34.8*aiWW + 10.0*aiB + 9.9*aiHW
15048  + 3.04*aiHB - 2.14*aiHQ + 31.1*aipHQ + 7.6*aiHu - 2.59*aiHd;
15049 
15050  return STXSb;
15051 }

◆ STXS_ZHqqHqq_VH2j()

double NPSMEFTd6::STXS_ZHqqHqq_VH2j ( const double  sqrt_s) const
virtual

The STXS bin \( qq \to ZH \to H qq \).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15063 of file NPSMEFTd6.cpp.

15063  {
15064 
15065  double STXSb = 1.0;
15066 
15067  STXSb = 1.0 - 0.998*aiH - 4.002*aiT + 37.99*aiWW + 10.47*aiB + 16.45*aiHW
15068  + 4.927*aiHB - 2.401*aiHQ + 34.45*aipHQ + 7.94*aiHu - 2.993*aiHd;
15069 
15070  return STXSb;
15071 }

◆ xseeWW()

double NPSMEFTd6::xseeWW ( const double  sqrt_s) const
virtual

Total \(e^+ e^- \to W^+ W^- \to jj \ell \nu\) cross section in pb, with \(\ell= e, \mu\).

Returns
\(\sigma(e^+ e^- \to W^+ W^- \to jj \ell \nu) \)

Reimplemented from NPbase.

Definition at line 13909 of file NPSMEFTd6.cpp.

13910 {
13911  return dxseeWWdcosBin(sqrt_s, -1.0, 1.0);
13912 }

Member Data Documentation

◆ ai2G

double NPSMEFTd6::ai2G
protected

Definition at line 4915 of file NPSMEFTd6.h.

◆ ai3G

double NPSMEFTd6::ai3G
protected

Definition at line 4915 of file NPSMEFTd6.h.

◆ aiA

double NPSMEFTd6::aiA
protected

Definition at line 4917 of file NPSMEFTd6.h.

◆ aiB

double NPSMEFTd6::aiB
protected

Definition at line 4916 of file NPSMEFTd6.h.

◆ aiG

double NPSMEFTd6::aiG
protected

Definition at line 4915 of file NPSMEFTd6.h.

◆ aiH

double NPSMEFTd6::aiH
protected

Definition at line 4916 of file NPSMEFTd6.h.

◆ aiHB

double NPSMEFTd6::aiHB
protected

Definition at line 4916 of file NPSMEFTd6.h.

◆ aiHd

double NPSMEFTd6::aiHd
protected

Definition at line 4918 of file NPSMEFTd6.h.

◆ aiHe

double NPSMEFTd6::aiHe
protected

Definition at line 4918 of file NPSMEFTd6.h.

◆ aiHL

double NPSMEFTd6::aiHL
protected

Definition at line 4918 of file NPSMEFTd6.h.

◆ aiHQ

double NPSMEFTd6::aiHQ
protected

Definition at line 4918 of file NPSMEFTd6.h.

◆ aiHu

double NPSMEFTd6::aiHu
protected

Definition at line 4918 of file NPSMEFTd6.h.

◆ aiHW

double NPSMEFTd6::aiHW
protected

Definition at line 4916 of file NPSMEFTd6.h.

◆ aipHL

double NPSMEFTd6::aipHL
protected

Definition at line 4918 of file NPSMEFTd6.h.

◆ aipHQ

double NPSMEFTd6::aipHQ
protected

Definition at line 4918 of file NPSMEFTd6.h.

◆ aiT

double NPSMEFTd6::aiT
protected

Definition at line 4916 of file NPSMEFTd6.h.

◆ aiu

double NPSMEFTd6::aiu
protected

Definition at line 4919 of file NPSMEFTd6.h.

◆ aiuG

double NPSMEFTd6::aiuG
protected

Definition at line 4919 of file NPSMEFTd6.h.

◆ aiWW

double NPSMEFTd6::aiWW
protected

Definition at line 4916 of file NPSMEFTd6.h.

◆ aleMz

double NPSMEFTd6::aleMz
protected

The em constant at Mz.

Definition at line 4875 of file NPSMEFTd6.h.

◆ BrHexo

double NPSMEFTd6::BrHexo
protected

The branching ratio of exotic (not invisible) Higgs decays.

Definition at line 4795 of file NPSMEFTd6.h.

◆ BrHinv

double NPSMEFTd6::BrHinv
protected

The branching ratio of invisible Higgs decays.

Definition at line 4794 of file NPSMEFTd6.h.

◆ C2B

double NPSMEFTd6::C2B
protected

The dimension-6 operator coefficient \(C_{2W}\).

Definition at line 4415 of file NPSMEFTd6.h.

◆ C2BS

double NPSMEFTd6::C2BS
protected

The dimension-6 operator coefficient \(C_{2W}^{SILH}\).

Definition at line 4417 of file NPSMEFTd6.h.

◆ C2W

double NPSMEFTd6::C2W
protected

The dimension-6 operator coefficient \(C_{2B}\).

Definition at line 4416 of file NPSMEFTd6.h.

◆ C2WS

double NPSMEFTd6::C2WS
protected

The dimension-6 operator coefficient \(C_{2B}^{SILH}\).

Definition at line 4418 of file NPSMEFTd6.h.

◆ CDB

double NPSMEFTd6::CDB
protected

The dimension-6 operator coefficient \(C_{DB}\).

Definition at line 4426 of file NPSMEFTd6.h.

◆ CdH_11i

double NPSMEFTd6::CdH_11i
protected

The dimension-6 operator coefficient \((C_{dH})_{11}\) (imaginary part).

Definition at line 4538 of file NPSMEFTd6.h.

◆ CdH_11r

double NPSMEFTd6::CdH_11r
protected

The dimension-6 operator coefficient \((C_{dH})_{11}\) (real part).

Definition at line 4532 of file NPSMEFTd6.h.

◆ CdH_12i

double NPSMEFTd6::CdH_12i
protected

The dimension-6 operator coefficient \((C_{dH})_{12}\) (imaginary part).

Definition at line 4539 of file NPSMEFTd6.h.

◆ CdH_12r

double NPSMEFTd6::CdH_12r
protected

The dimension-6 operator coefficient \((C_{dH})_{12}\) (real part).

Definition at line 4533 of file NPSMEFTd6.h.

◆ CdH_13i

double NPSMEFTd6::CdH_13i
protected

The dimension-6 operator coefficient \((C_{dH})_{13}\) (imaginary part).

Definition at line 4540 of file NPSMEFTd6.h.

◆ CdH_13r

double NPSMEFTd6::CdH_13r
protected

The dimension-6 operator coefficient \((C_{dH})_{13}\) (real part).

Definition at line 4534 of file NPSMEFTd6.h.

◆ CdH_22i

double NPSMEFTd6::CdH_22i
protected

The dimension-6 operator coefficient \((C_{dH})_{22}\) (imaginary part).

Definition at line 4541 of file NPSMEFTd6.h.

◆ CdH_22r

double NPSMEFTd6::CdH_22r
protected

The dimension-6 operator coefficient \((C_{dH})_{22}\) (real part).

Definition at line 4535 of file NPSMEFTd6.h.

◆ CdH_23i

double NPSMEFTd6::CdH_23i
protected

The dimension-6 operator coefficient \((C_{dH})_{23}\) (imaginary part).

Definition at line 4542 of file NPSMEFTd6.h.

◆ CdH_23r

double NPSMEFTd6::CdH_23r
protected

The dimension-6 operator coefficient \((C_{dH})_{23}\) (real part).

Definition at line 4536 of file NPSMEFTd6.h.

◆ CdH_33i

double NPSMEFTd6::CdH_33i
protected

The dimension-6 operator coefficient \((C_{dH})_{33}\) (imaginary part).

Definition at line 4543 of file NPSMEFTd6.h.

◆ CdH_33r

double NPSMEFTd6::CdH_33r
protected

The dimension-6 operator coefficient \((C_{dH})_{33}\) (real part).

Definition at line 4537 of file NPSMEFTd6.h.

◆ CDHB

double NPSMEFTd6::CDHB
protected

The dimension-6 operator coefficient \(C_{DHB}\).

Definition at line 4424 of file NPSMEFTd6.h.

◆ CDHW

double NPSMEFTd6::CDHW
protected

The dimension-6 operator coefficient \(C_{DHW}\).

Definition at line 4425 of file NPSMEFTd6.h.

◆ CDW

double NPSMEFTd6::CDW
protected

The dimension-6 operator coefficient \(C_{DW}\).

Definition at line 4427 of file NPSMEFTd6.h.

◆ Ced_1111

double NPSMEFTd6::Ced_1111
protected

Definition at line 4600 of file NPSMEFTd6.h.

◆ Ced_1122

double NPSMEFTd6::Ced_1122
protected

Definition at line 4601 of file NPSMEFTd6.h.

◆ Ced_1123

double NPSMEFTd6::Ced_1123
protected

Definition at line 4603 of file NPSMEFTd6.h.

◆ Ced_1132

double NPSMEFTd6::Ced_1132
protected

Definition at line 4604 of file NPSMEFTd6.h.

◆ Ced_1133

double NPSMEFTd6::Ced_1133
protected

Definition at line 4602 of file NPSMEFTd6.h.

◆ Ced_2211

double NPSMEFTd6::Ced_2211
protected

Definition at line 4601 of file NPSMEFTd6.h.

◆ Ced_2223

double NPSMEFTd6::Ced_2223
protected

Definition at line 4603 of file NPSMEFTd6.h.

◆ Ced_2232

double NPSMEFTd6::Ced_2232
protected

Definition at line 4604 of file NPSMEFTd6.h.

◆ Ced_3311

double NPSMEFTd6::Ced_3311
protected

Definition at line 4602 of file NPSMEFTd6.h.

◆ Ced_3323

double NPSMEFTd6::Ced_3323
protected

Definition at line 4603 of file NPSMEFTd6.h.

◆ Ced_3332

double NPSMEFTd6::Ced_3332
protected

Definition at line 4604 of file NPSMEFTd6.h.

◆ Cee_1111

double NPSMEFTd6::Cee_1111
protected

Definition at line 4593 of file NPSMEFTd6.h.

◆ Cee_1122

double NPSMEFTd6::Cee_1122
protected

Definition at line 4594 of file NPSMEFTd6.h.

◆ Cee_1133

double NPSMEFTd6::Cee_1133
protected

Definition at line 4595 of file NPSMEFTd6.h.

◆ Cee_2211

double NPSMEFTd6::Cee_2211
protected

Definition at line 4594 of file NPSMEFTd6.h.

◆ Cee_3311

double NPSMEFTd6::Cee_3311
protected

Definition at line 4595 of file NPSMEFTd6.h.

◆ CeH_11i

double NPSMEFTd6::CeH_11i
protected

The dimension-6 operator coefficient \((C_{eH})_{11}\) (imaginary part).

Definition at line 4514 of file NPSMEFTd6.h.

◆ CeH_11r

double NPSMEFTd6::CeH_11r
protected

The dimension-6 operator coefficient \((C_{eH})_{11}\) (real part).

Definition at line 4508 of file NPSMEFTd6.h.

◆ CeH_12i

double NPSMEFTd6::CeH_12i
protected

The dimension-6 operator coefficient \((C_{eH})_{12}\) (imaginary part).

Definition at line 4515 of file NPSMEFTd6.h.

◆ CeH_12r

double NPSMEFTd6::CeH_12r
protected

The dimension-6 operator coefficient \((C_{eH})_{12}\) (real part).

Definition at line 4509 of file NPSMEFTd6.h.

◆ CeH_13i

double NPSMEFTd6::CeH_13i
protected

The dimension-6 operator coefficient \((C_{eH})_{13}\) (imaginary part).

Definition at line 4516 of file NPSMEFTd6.h.

◆ CeH_13r

double NPSMEFTd6::CeH_13r
protected

The dimension-6 operator coefficient \((C_{eH})_{13}\) (real part).

Definition at line 4510 of file NPSMEFTd6.h.

◆ CeH_22i

double NPSMEFTd6::CeH_22i
protected

The dimension-6 operator coefficient \((C_{eH})_{22}\) (imaginary part).

Definition at line 4517 of file NPSMEFTd6.h.

◆ CeH_22r

double NPSMEFTd6::CeH_22r
protected

The dimension-6 operator coefficient \((C_{eH})_{22}\) (real part).

Definition at line 4511 of file NPSMEFTd6.h.

◆ CeH_23i

double NPSMEFTd6::CeH_23i
protected

The dimension-6 operator coefficient \((C_{eH})_{23}\) (imaginary part).

Definition at line 4518 of file NPSMEFTd6.h.

◆ CeH_23r

double NPSMEFTd6::CeH_23r
protected

The dimension-6 operator coefficient \((C_{eH})_{23}\) (real part).

Definition at line 4512 of file NPSMEFTd6.h.

◆ CeH_33i

double NPSMEFTd6::CeH_33i
protected

The dimension-6 operator coefficient \((C_{eH})_{33}\) (imaginary part).

Definition at line 4519 of file NPSMEFTd6.h.

◆ CeH_33r

double NPSMEFTd6::CeH_33r
protected

The dimension-6 operator coefficient \((C_{eH})_{33}\) (real part).

Definition at line 4513 of file NPSMEFTd6.h.

◆ Ceu_1111

double NPSMEFTd6::Ceu_1111
protected

Definition at line 4596 of file NPSMEFTd6.h.

◆ Ceu_1122

double NPSMEFTd6::Ceu_1122
protected

Definition at line 4597 of file NPSMEFTd6.h.

◆ Ceu_1133

double NPSMEFTd6::Ceu_1133
protected

Definition at line 4598 of file NPSMEFTd6.h.

◆ Ceu_2211

double NPSMEFTd6::Ceu_2211
protected

Definition at line 4597 of file NPSMEFTd6.h.

◆ Ceu_2233

double NPSMEFTd6::Ceu_2233
protected

Definition at line 4599 of file NPSMEFTd6.h.

◆ Ceu_3311

double NPSMEFTd6::Ceu_3311
protected

Definition at line 4598 of file NPSMEFTd6.h.

◆ CG

double NPSMEFTd6::CG
protected

The dimension-6 operator coefficient \(C_{G}\).

Definition at line 4413 of file NPSMEFTd6.h.

◆ CH

double NPSMEFTd6::CH
protected

The dimension-6 operator coefficient \(C_{H}\).

Definition at line 4432 of file NPSMEFTd6.h.

◆ CHB

double NPSMEFTd6::CHB
protected

The dimension-6 operator coefficient \(C_{HB}\).

Definition at line 4421 of file NPSMEFTd6.h.

◆ CHbox

double NPSMEFTd6::CHbox
protected

The dimension-6 operator coefficient \(C_{H\Box}\).

Definition at line 4431 of file NPSMEFTd6.h.

◆ CHD

double NPSMEFTd6::CHD
protected

The dimension-6 operator coefficient \(C_{HD}\).

Definition at line 4429 of file NPSMEFTd6.h.

◆ CHd_11

double NPSMEFTd6::CHd_11
protected

The dimension-6 operator coefficient \((C_{Hd})_{11}\).

Definition at line 4487 of file NPSMEFTd6.h.

◆ CHd_12i

double NPSMEFTd6::CHd_12i
protected

The dimension-6 operator coefficient \((C_{Hd})_{12}\) (imaginary part).

Definition at line 4493 of file NPSMEFTd6.h.

◆ CHd_12r

double NPSMEFTd6::CHd_12r
protected

The dimension-6 operator coefficient \((C_{Hd})_{12}\) (real part).

Definition at line 4488 of file NPSMEFTd6.h.

◆ CHd_13i

double NPSMEFTd6::CHd_13i
protected

The dimension-6 operator coefficient \((C_{Hd})_{13}\) (imaginary part).

Definition at line 4494 of file NPSMEFTd6.h.

◆ CHd_13r

double NPSMEFTd6::CHd_13r
protected

The dimension-6 operator coefficient \((C_{Hd})_{13}\) (real part).

Definition at line 4489 of file NPSMEFTd6.h.

◆ CHd_22

double NPSMEFTd6::CHd_22
protected

The dimension-6 operator coefficient \((C_{Hd})_{22}\).

Definition at line 4490 of file NPSMEFTd6.h.

◆ CHd_23i

double NPSMEFTd6::CHd_23i
protected

The dimension-6 operator coefficient \((C_{Hd})_{23}\) (imaginary part).

Definition at line 4495 of file NPSMEFTd6.h.

◆ CHd_23r

double NPSMEFTd6::CHd_23r
protected

The dimension-6 operator coefficient \((C_{Hd})_{23}\) (real part).

Definition at line 4491 of file NPSMEFTd6.h.

◆ CHd_33

double NPSMEFTd6::CHd_33
protected

The dimension-6 operator coefficient \((C_{Hd})_{33}\).

Definition at line 4492 of file NPSMEFTd6.h.

◆ CHe_11

double NPSMEFTd6::CHe_11
protected

The dimension-6 operator coefficient \((C_{He})_{11}\).

Definition at line 4451 of file NPSMEFTd6.h.

◆ CHe_12i

double NPSMEFTd6::CHe_12i
protected

The dimension-6 operator coefficient \((C_{He})_{12}\) (imaginary part).

Definition at line 4457 of file NPSMEFTd6.h.

◆ CHe_12r

double NPSMEFTd6::CHe_12r
protected

The dimension-6 operator coefficient \((C_{He})_{12}\) (real part).

Definition at line 4452 of file NPSMEFTd6.h.

◆ CHe_13i

double NPSMEFTd6::CHe_13i
protected

The dimension-6 operator coefficient \((C_{He})_{13}\) (imaginary part).

Definition at line 4458 of file NPSMEFTd6.h.

◆ CHe_13r

double NPSMEFTd6::CHe_13r
protected

The dimension-6 operator coefficient \((C_{He})_{13}\) (real part).

Definition at line 4453 of file NPSMEFTd6.h.

◆ CHe_22

double NPSMEFTd6::CHe_22
protected

The dimension-6 operator coefficient \((C_{He})_{22}\).

Definition at line 4454 of file NPSMEFTd6.h.

◆ CHe_23i

double NPSMEFTd6::CHe_23i
protected

The dimension-6 operator coefficient \((C_{He})_{23}\) (imaginary part).

Definition at line 4459 of file NPSMEFTd6.h.

◆ CHe_23r

double NPSMEFTd6::CHe_23r
protected

The dimension-6 operator coefficient \((C_{He})_{23}\) (real part).

Definition at line 4455 of file NPSMEFTd6.h.

◆ CHe_33

double NPSMEFTd6::CHe_33
protected

The dimension-6 operator coefficient \((C_{He})_{33}\).

Definition at line 4456 of file NPSMEFTd6.h.

◆ CHG

double NPSMEFTd6::CHG
protected

The dimension-6 operator coefficient \(C_{HG}\).

Definition at line 4419 of file NPSMEFTd6.h.

◆ CHL1_11

double NPSMEFTd6::CHL1_11
protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{11}\).

Definition at line 4433 of file NPSMEFTd6.h.

◆ CHL1_12i

double NPSMEFTd6::CHL1_12i
protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (imaginary part).

Definition at line 4439 of file NPSMEFTd6.h.

◆ CHL1_12r

double NPSMEFTd6::CHL1_12r
protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (real part).

Definition at line 4434 of file NPSMEFTd6.h.

◆ CHL1_13i

double NPSMEFTd6::CHL1_13i
protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (imaginary part).

Definition at line 4440 of file NPSMEFTd6.h.

◆ CHL1_13r

double NPSMEFTd6::CHL1_13r
protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (real part).

Definition at line 4435 of file NPSMEFTd6.h.

◆ CHL1_22

double NPSMEFTd6::CHL1_22
protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{22}\).

Definition at line 4436 of file NPSMEFTd6.h.

◆ CHL1_23i

double NPSMEFTd6::CHL1_23i
protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (imaginary part).

Definition at line 4441 of file NPSMEFTd6.h.

◆ CHL1_23r

double NPSMEFTd6::CHL1_23r
protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (real part).

Definition at line 4437 of file NPSMEFTd6.h.

◆ CHL1_33

double NPSMEFTd6::CHL1_33
protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{33}\).

Definition at line 4438 of file NPSMEFTd6.h.

◆ CHL3_11

double NPSMEFTd6::CHL3_11
protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{11}\).

Definition at line 4442 of file NPSMEFTd6.h.

◆ CHL3_12i

double NPSMEFTd6::CHL3_12i
protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part).

Definition at line 4448 of file NPSMEFTd6.h.

◆ CHL3_12r

double NPSMEFTd6::CHL3_12r
protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part).

Definition at line 4443 of file NPSMEFTd6.h.

◆ CHL3_13i

double NPSMEFTd6::CHL3_13i
protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part).

Definition at line 4449 of file NPSMEFTd6.h.

◆ CHL3_13r

double NPSMEFTd6::CHL3_13r
protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part).

Definition at line 4444 of file NPSMEFTd6.h.

◆ CHL3_22

double NPSMEFTd6::CHL3_22
protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{22}\).

Definition at line 4445 of file NPSMEFTd6.h.

◆ CHL3_23i

double NPSMEFTd6::CHL3_23i
protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part).

Definition at line 4450 of file NPSMEFTd6.h.

◆ CHL3_23r

double NPSMEFTd6::CHL3_23r
protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part).

Definition at line 4446 of file NPSMEFTd6.h.

◆ CHL3_33

double NPSMEFTd6::CHL3_33
protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{33}\).

Definition at line 4447 of file NPSMEFTd6.h.

◆ CHQ1_11

double NPSMEFTd6::CHQ1_11
protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{11}\).

Definition at line 4460 of file NPSMEFTd6.h.

◆ CHQ1_12i

double NPSMEFTd6::CHQ1_12i
protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (imaginary part).

Definition at line 4466 of file NPSMEFTd6.h.

◆ CHQ1_12r

double NPSMEFTd6::CHQ1_12r
protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (real part).

Definition at line 4461 of file NPSMEFTd6.h.

◆ CHQ1_13i

double NPSMEFTd6::CHQ1_13i
protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (imaginary part).

Definition at line 4467 of file NPSMEFTd6.h.

◆ CHQ1_13r

double NPSMEFTd6::CHQ1_13r
protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (real part).

Definition at line 4462 of file NPSMEFTd6.h.

◆ CHQ1_22

double NPSMEFTd6::CHQ1_22
protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{22}\).

Definition at line 4463 of file NPSMEFTd6.h.

◆ CHQ1_23i

double NPSMEFTd6::CHQ1_23i
protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (imaginary part).

Definition at line 4468 of file NPSMEFTd6.h.

◆ CHQ1_23r

double NPSMEFTd6::CHQ1_23r
protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (real part).

Definition at line 4464 of file NPSMEFTd6.h.

◆ CHQ1_33

double NPSMEFTd6::CHQ1_33
protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{33}\).

Definition at line 4465 of file NPSMEFTd6.h.

◆ CHQ3_11

double NPSMEFTd6::CHQ3_11
protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{11}\).

Definition at line 4469 of file NPSMEFTd6.h.

◆ CHQ3_12i

double NPSMEFTd6::CHQ3_12i
protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (imaginary part).

Definition at line 4475 of file NPSMEFTd6.h.

◆ CHQ3_12r

double NPSMEFTd6::CHQ3_12r
protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (real part).

Definition at line 4470 of file NPSMEFTd6.h.

◆ CHQ3_13i

double NPSMEFTd6::CHQ3_13i
protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (imaginary part).

Definition at line 4476 of file NPSMEFTd6.h.

◆ CHQ3_13r

double NPSMEFTd6::CHQ3_13r
protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (real part).

Definition at line 4471 of file NPSMEFTd6.h.

◆ CHQ3_22

double NPSMEFTd6::CHQ3_22
protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{22}\).

Definition at line 4472 of file NPSMEFTd6.h.

◆ CHQ3_23i

double NPSMEFTd6::CHQ3_23i
protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (imaginary part).

Definition at line 4477 of file NPSMEFTd6.h.

◆ CHQ3_23r

double NPSMEFTd6::CHQ3_23r
protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (real part).

Definition at line 4473 of file NPSMEFTd6.h.

◆ CHQ3_33

double NPSMEFTd6::CHQ3_33
protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{33}\).

Definition at line 4474 of file NPSMEFTd6.h.

◆ cHSM

double NPSMEFTd6::cHSM
protected

Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes.

Definition at line 4904 of file NPSMEFTd6.h.

◆ CHu_11

double NPSMEFTd6::CHu_11
protected

The dimension-6 operator coefficient \((C_{Hu})_{11}\).

Definition at line 4478 of file NPSMEFTd6.h.

◆ CHu_12i

double NPSMEFTd6::CHu_12i
protected

The dimension-6 operator coefficient \((C_{Hu})_{12}\) (imaginary part).

Definition at line 4484 of file NPSMEFTd6.h.

◆ CHu_12r

double NPSMEFTd6::CHu_12r
protected

The dimension-6 operator coefficient \((C_{Hu})_{12}\) (real part).

Definition at line 4479 of file NPSMEFTd6.h.

◆ CHu_13i

double NPSMEFTd6::CHu_13i
protected

The dimension-6 operator coefficient \((C_{Hu})_{13}\) (imaginary part).

Definition at line 4485 of file NPSMEFTd6.h.

◆ CHu_13r

double NPSMEFTd6::CHu_13r
protected

The dimension-6 operator coefficient \((C_{Hu})_{13}\) (real part).

Definition at line 4480 of file NPSMEFTd6.h.

◆ CHu_22

double NPSMEFTd6::CHu_22
protected

The dimension-6 operator coefficient \((C_{Hu})_{22}\).

Definition at line 4481 of file NPSMEFTd6.h.

◆ CHu_23i

double NPSMEFTd6::CHu_23i
protected

The dimension-6 operator coefficient \((C_{Hu})_{23}\) (imaginary part).

Definition at line 4486 of file NPSMEFTd6.h.

◆ CHu_23r

double NPSMEFTd6::CHu_23r
protected

The dimension-6 operator coefficient \((C_{Hu})_{23}\) (real part).

Definition at line 4482 of file NPSMEFTd6.h.

◆ CHu_33

double NPSMEFTd6::CHu_33
protected

The dimension-6 operator coefficient \((C_{Hu})_{33}\).

Definition at line 4483 of file NPSMEFTd6.h.

◆ CHud_11i

double NPSMEFTd6::CHud_11i
protected

The dimension-6 operator coefficient \((C_{Hud})_{11}\) (imaginary part).

Definition at line 4502 of file NPSMEFTd6.h.

◆ CHud_11r

double NPSMEFTd6::CHud_11r
protected

The dimension-6 operator coefficient \((C_{Hud})_{11}\) (real part).

Definition at line 4496 of file NPSMEFTd6.h.

◆ CHud_12i

double NPSMEFTd6::CHud_12i
protected

The dimension-6 operator coefficient \((C_{Hud})_{12}\) (imaginary part).

Definition at line 4503 of file NPSMEFTd6.h.

◆ CHud_12r

double NPSMEFTd6::CHud_12r
protected

The dimension-6 operator coefficient \((C_{Hud})_{12}\) (real part).

Definition at line 4497 of file NPSMEFTd6.h.

◆ CHud_13i

double NPSMEFTd6::CHud_13i
protected

The dimension-6 operator coefficient \((C_{Hud})_{13}\) (imaginary part).

Definition at line 4504 of file NPSMEFTd6.h.

◆ CHud_13r

double NPSMEFTd6::CHud_13r
protected

The dimension-6 operator coefficient \((C_{Hud})_{13}\) (real part).

Definition at line 4498 of file NPSMEFTd6.h.

◆ CHud_22i

double NPSMEFTd6::CHud_22i
protected

The dimension-6 operator coefficient \((C_{Hud})_{22}\) (imaginary part).

Definition at line 4505 of file NPSMEFTd6.h.

◆ CHud_22r

double NPSMEFTd6::CHud_22r
protected

The dimension-6 operator coefficient \((C_{Hud})_{22}\) (real part).

Definition at line 4499 of file NPSMEFTd6.h.

◆ CHud_23i

double NPSMEFTd6::CHud_23i
protected

The dimension-6 operator coefficient \((C_{Hud})_{23}\) (imaginary part).

Definition at line 4506 of file NPSMEFTd6.h.

◆ CHud_23r

double NPSMEFTd6::CHud_23r
protected

The dimension-6 operator coefficient \((C_{Hud})_{23}\) (real part).

Definition at line 4500 of file NPSMEFTd6.h.

◆ CHud_33i

double NPSMEFTd6::CHud_33i
protected

The dimension-6 operator coefficient \((C_{Hud})_{33}\) (imaginary part).

Definition at line 4507 of file NPSMEFTd6.h.

◆ CHud_33r

double NPSMEFTd6::CHud_33r
protected

The dimension-6 operator coefficient \((C_{Hud})_{33}\) (real part).

Definition at line 4501 of file NPSMEFTd6.h.

◆ CHW

double NPSMEFTd6::CHW
protected

The dimension-6 operator coefficient \(C_{HW}\).

Definition at line 4420 of file NPSMEFTd6.h.

◆ CHWB

double NPSMEFTd6::CHWB
protected

The dimension-6 operator coefficient \(C_{HWB}\).

Definition at line 4428 of file NPSMEFTd6.h.

◆ CHWHB_gaga

double NPSMEFTd6::CHWHB_gaga
protected

The combination of dimension-6 operator coefficients entering in \(\delta_{AA}\): \(s_W^2 C_{HW} + c_W^2 C_{HW}\).

Definition at line 4422 of file NPSMEFTd6.h.

◆ CHWHB_gagaorth

double NPSMEFTd6::CHWHB_gagaorth
protected

The combination of dimension-6 operator coefficients \(-c_W^2 C_{HW} + s_W^2 C_{HW}\).

Definition at line 4423 of file NPSMEFTd6.h.

◆ CidH_11r

double NPSMEFTd6::CidH_11r
protected

Definition at line 4854 of file NPSMEFTd6.h.

◆ CidH_22r

double NPSMEFTd6::CidH_22r
protected

Definition at line 4855 of file NPSMEFTd6.h.

◆ CidH_33r

double NPSMEFTd6::CidH_33r
protected

Definition at line 4856 of file NPSMEFTd6.h.

◆ CiDHB

double NPSMEFTd6::CiDHB
protected

Definition at line 4838 of file NPSMEFTd6.h.

◆ CiDHW

double NPSMEFTd6::CiDHW
protected

Definition at line 4839 of file NPSMEFTd6.h.

◆ CieH_11r

double NPSMEFTd6::CieH_11r
protected

Definition at line 4846 of file NPSMEFTd6.h.

◆ CieH_22r

double NPSMEFTd6::CieH_22r
protected

Definition at line 4847 of file NPSMEFTd6.h.

◆ CieH_33r

double NPSMEFTd6::CieH_33r
protected

Definition at line 4848 of file NPSMEFTd6.h.

◆ CiH

double NPSMEFTd6::CiH
protected

Definition at line 4844 of file NPSMEFTd6.h.

◆ CiHB

double NPSMEFTd6::CiHB
protected

Definition at line 4837 of file NPSMEFTd6.h.

◆ CiHbox

double NPSMEFTd6::CiHbox
protected

Definition at line 4842 of file NPSMEFTd6.h.

◆ CiHD

double NPSMEFTd6::CiHD
protected

Definition at line 4843 of file NPSMEFTd6.h.

◆ CiHd_11

double NPSMEFTd6::CiHd_11
protected

Definition at line 4830 of file NPSMEFTd6.h.

◆ CiHd_22

double NPSMEFTd6::CiHd_22
protected

Definition at line 4831 of file NPSMEFTd6.h.

◆ CiHd_33

double NPSMEFTd6::CiHd_33
protected

Definition at line 4832 of file NPSMEFTd6.h.

◆ CiHe_11

double NPSMEFTd6::CiHe_11
protected

Definition at line 4822 of file NPSMEFTd6.h.

◆ CiHe_22

double NPSMEFTd6::CiHe_22
protected

Definition at line 4823 of file NPSMEFTd6.h.

◆ CiHe_33

double NPSMEFTd6::CiHe_33
protected

Definition at line 4824 of file NPSMEFTd6.h.

◆ CiHL1_11

double NPSMEFTd6::CiHL1_11
protected

Definition at line 4808 of file NPSMEFTd6.h.

◆ CiHL1_22

double NPSMEFTd6::CiHL1_22
protected

Definition at line 4809 of file NPSMEFTd6.h.

◆ CiHL1_33

double NPSMEFTd6::CiHL1_33
protected

Definition at line 4810 of file NPSMEFTd6.h.

◆ CiHL3_11

double NPSMEFTd6::CiHL3_11
protected

Definition at line 4811 of file NPSMEFTd6.h.

◆ CiHL3_22

double NPSMEFTd6::CiHL3_22
protected

Definition at line 4812 of file NPSMEFTd6.h.

◆ CiHL3_33

double NPSMEFTd6::CiHL3_33
protected

Definition at line 4813 of file NPSMEFTd6.h.

◆ CiHQ1_11

double NPSMEFTd6::CiHQ1_11
protected

Definition at line 4815 of file NPSMEFTd6.h.

◆ CiHQ1_22

double NPSMEFTd6::CiHQ1_22
protected

Definition at line 4816 of file NPSMEFTd6.h.

◆ CiHQ1_33

double NPSMEFTd6::CiHQ1_33
protected

Definition at line 4817 of file NPSMEFTd6.h.

◆ CiHQ3_11

double NPSMEFTd6::CiHQ3_11
protected

Definition at line 4818 of file NPSMEFTd6.h.

◆ CiHQ3_22

double NPSMEFTd6::CiHQ3_22
protected

Definition at line 4819 of file NPSMEFTd6.h.

◆ CiHQ3_33

double NPSMEFTd6::CiHQ3_33
protected

Definition at line 4820 of file NPSMEFTd6.h.

◆ CiHu_11

double NPSMEFTd6::CiHu_11
protected

Definition at line 4826 of file NPSMEFTd6.h.

◆ CiHu_22

double NPSMEFTd6::CiHu_22
protected

Definition at line 4827 of file NPSMEFTd6.h.

◆ CiHu_33

double NPSMEFTd6::CiHu_33
protected

Definition at line 4828 of file NPSMEFTd6.h.

◆ CiHW

double NPSMEFTd6::CiHW
protected

Definition at line 4836 of file NPSMEFTd6.h.

◆ CiHWB

double NPSMEFTd6::CiHWB
protected

Definition at line 4840 of file NPSMEFTd6.h.

◆ CiLL_1221

double NPSMEFTd6::CiLL_1221
protected

Definition at line 4870 of file NPSMEFTd6.h.

◆ CiLL_2112

double NPSMEFTd6::CiLL_2112
protected

Definition at line 4871 of file NPSMEFTd6.h.

◆ CiuB_11r

double NPSMEFTd6::CiuB_11r
protected

Definition at line 4866 of file NPSMEFTd6.h.

◆ CiuB_22r

double NPSMEFTd6::CiuB_22r
protected

Definition at line 4867 of file NPSMEFTd6.h.

◆ CiuB_33r

double NPSMEFTd6::CiuB_33r
protected

Definition at line 4868 of file NPSMEFTd6.h.

◆ CiuG_11r

double NPSMEFTd6::CiuG_11r
protected

Definition at line 4858 of file NPSMEFTd6.h.

◆ CiuG_22r

double NPSMEFTd6::CiuG_22r
protected

Definition at line 4859 of file NPSMEFTd6.h.

◆ CiuG_33r

double NPSMEFTd6::CiuG_33r
protected

Definition at line 4860 of file NPSMEFTd6.h.

◆ CiuH_11r

double NPSMEFTd6::CiuH_11r
protected

Definition at line 4850 of file NPSMEFTd6.h.

◆ CiuH_22r

double NPSMEFTd6::CiuH_22r
protected

Definition at line 4851 of file NPSMEFTd6.h.

◆ CiuH_33r

double NPSMEFTd6::CiuH_33r
protected

Definition at line 4852 of file NPSMEFTd6.h.

◆ CiuW_11r

double NPSMEFTd6::CiuW_11r
protected

Definition at line 4862 of file NPSMEFTd6.h.

◆ CiuW_22r

double NPSMEFTd6::CiuW_22r
protected

Definition at line 4863 of file NPSMEFTd6.h.

◆ CiuW_33r

double NPSMEFTd6::CiuW_33r
protected

Definition at line 4864 of file NPSMEFTd6.h.

◆ CiW

double NPSMEFTd6::CiW
protected

Definition at line 4834 of file NPSMEFTd6.h.

◆ CLd_1111

double NPSMEFTd6::CLd_1111
protected

Definition at line 4612 of file NPSMEFTd6.h.

◆ CLd_1122

double NPSMEFTd6::CLd_1122
protected

Definition at line 4613 of file NPSMEFTd6.h.

◆ CLd_1123

double NPSMEFTd6::CLd_1123
protected

Definition at line 4615 of file NPSMEFTd6.h.

◆ CLd_1132

double NPSMEFTd6::CLd_1132
protected

Definition at line 4616 of file NPSMEFTd6.h.

◆ CLd_1133

double NPSMEFTd6::CLd_1133
protected

Definition at line 4614 of file NPSMEFTd6.h.

◆ CLd_2211

double NPSMEFTd6::CLd_2211
protected

Definition at line 4613 of file NPSMEFTd6.h.

◆ CLd_2223

double NPSMEFTd6::CLd_2223
protected

Definition at line 4615 of file NPSMEFTd6.h.

◆ CLd_2232

double NPSMEFTd6::CLd_2232
protected

Definition at line 4616 of file NPSMEFTd6.h.

◆ CLd_3311

double NPSMEFTd6::CLd_3311
protected

Definition at line 4614 of file NPSMEFTd6.h.

◆ CLd_3323

double NPSMEFTd6::CLd_3323
protected

Definition at line 4615 of file NPSMEFTd6.h.

◆ CLd_3332

double NPSMEFTd6::CLd_3332
protected

Definition at line 4616 of file NPSMEFTd6.h.

◆ CLe_1111

double NPSMEFTd6::CLe_1111
protected

Definition at line 4605 of file NPSMEFTd6.h.

◆ CLe_1122

double NPSMEFTd6::CLe_1122
protected

Definition at line 4606 of file NPSMEFTd6.h.

◆ CLe_1133

double NPSMEFTd6::CLe_1133
protected

Definition at line 4607 of file NPSMEFTd6.h.

◆ CLe_2211

double NPSMEFTd6::CLe_2211
protected

Definition at line 4606 of file NPSMEFTd6.h.

◆ CLe_3311

double NPSMEFTd6::CLe_3311
protected

Definition at line 4607 of file NPSMEFTd6.h.

◆ CLedQ_11

double NPSMEFTd6::CLedQ_11
protected

Definition at line 4622 of file NPSMEFTd6.h.

◆ CLedQ_22

double NPSMEFTd6::CLedQ_22
protected

Definition at line 4622 of file NPSMEFTd6.h.

◆ cLH3d62

double NPSMEFTd6::cLH3d62
protected

Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 interactions modifying the Higgs trilinear coupling (Quadratic terms).

Definition at line 4908 of file NPSMEFTd6.h.

◆ cLHd6

double NPSMEFTd6::cLHd6
protected

Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 interactions.

Definition at line 4906 of file NPSMEFTd6.h.

◆ CLL_1111

double NPSMEFTd6::CLL_1111
protected

Definition at line 4580 of file NPSMEFTd6.h.

◆ CLL_1122

double NPSMEFTd6::CLL_1122
protected

Definition at line 4581 of file NPSMEFTd6.h.

◆ CLL_1133

double NPSMEFTd6::CLL_1133
protected

Definition at line 4582 of file NPSMEFTd6.h.

◆ CLL_1221

double NPSMEFTd6::CLL_1221
protected

Definition at line 4581 of file NPSMEFTd6.h.

◆ CLL_1331

double NPSMEFTd6::CLL_1331
protected

Definition at line 4582 of file NPSMEFTd6.h.

◆ CLL_2112

double NPSMEFTd6::CLL_2112
protected

Definition at line 4581 of file NPSMEFTd6.h.

◆ CLL_2211

double NPSMEFTd6::CLL_2211
protected

Definition at line 4581 of file NPSMEFTd6.h.

◆ CLL_3113

double NPSMEFTd6::CLL_3113
protected

Definition at line 4582 of file NPSMEFTd6.h.

◆ CLL_3311

double NPSMEFTd6::CLL_3311
protected

Definition at line 4582 of file NPSMEFTd6.h.

◆ CLQ1_1111

double NPSMEFTd6::CLQ1_1111
protected

Definition at line 4583 of file NPSMEFTd6.h.

◆ CLQ1_1122

double NPSMEFTd6::CLQ1_1122
protected

Definition at line 4584 of file NPSMEFTd6.h.

◆ CLQ1_1123

double NPSMEFTd6::CLQ1_1123
protected

Definition at line 4586 of file NPSMEFTd6.h.

◆ CLQ1_1132

double NPSMEFTd6::CLQ1_1132
protected

Definition at line 4587 of file NPSMEFTd6.h.

◆ CLQ1_1133

double NPSMEFTd6::CLQ1_1133
protected

Definition at line 4585 of file NPSMEFTd6.h.

◆ CLQ1_1221

double NPSMEFTd6::CLQ1_1221
protected

Definition at line 4584 of file NPSMEFTd6.h.

◆ CLQ1_1331

double NPSMEFTd6::CLQ1_1331
protected

Definition at line 4585 of file NPSMEFTd6.h.

◆ CLQ1_2112

double NPSMEFTd6::CLQ1_2112
protected

Definition at line 4584 of file NPSMEFTd6.h.

◆ CLQ1_2211

double NPSMEFTd6::CLQ1_2211
protected

Definition at line 4584 of file NPSMEFTd6.h.

◆ CLQ1_2223

double NPSMEFTd6::CLQ1_2223
protected

Definition at line 4586 of file NPSMEFTd6.h.

◆ CLQ1_2232

double NPSMEFTd6::CLQ1_2232
protected

Definition at line 4587 of file NPSMEFTd6.h.

◆ CLQ1_3113

double NPSMEFTd6::CLQ1_3113
protected

Definition at line 4585 of file NPSMEFTd6.h.

◆ CLQ1_3311

double NPSMEFTd6::CLQ1_3311
protected

Definition at line 4585 of file NPSMEFTd6.h.

◆ CLQ1_3323

double NPSMEFTd6::CLQ1_3323
protected

Definition at line 4586 of file NPSMEFTd6.h.

◆ CLQ1_3332

double NPSMEFTd6::CLQ1_3332
protected

Definition at line 4587 of file NPSMEFTd6.h.

◆ CLQ3_1111

double NPSMEFTd6::CLQ3_1111
protected

Definition at line 4588 of file NPSMEFTd6.h.

◆ CLQ3_1122

double NPSMEFTd6::CLQ3_1122
protected

Definition at line 4589 of file NPSMEFTd6.h.

◆ CLQ3_1123

double NPSMEFTd6::CLQ3_1123
protected

Definition at line 4591 of file NPSMEFTd6.h.

◆ CLQ3_1132

double NPSMEFTd6::CLQ3_1132
protected

Definition at line 4592 of file NPSMEFTd6.h.

◆ CLQ3_1133

double NPSMEFTd6::CLQ3_1133
protected

Definition at line 4590 of file NPSMEFTd6.h.

◆ CLQ3_1221

double NPSMEFTd6::CLQ3_1221
protected

Definition at line 4589 of file NPSMEFTd6.h.

◆ CLQ3_1331

double NPSMEFTd6::CLQ3_1331
protected

Definition at line 4590 of file NPSMEFTd6.h.

◆ CLQ3_2112

double NPSMEFTd6::CLQ3_2112
protected

Definition at line 4589 of file NPSMEFTd6.h.

◆ CLQ3_2211

double NPSMEFTd6::CLQ3_2211
protected

Definition at line 4589 of file NPSMEFTd6.h.

◆ CLQ3_2223

double NPSMEFTd6::CLQ3_2223
protected

Definition at line 4591 of file NPSMEFTd6.h.

◆ CLQ3_2232

double NPSMEFTd6::CLQ3_2232
protected

Definition at line 4592 of file NPSMEFTd6.h.

◆ CLQ3_3113

double NPSMEFTd6::CLQ3_3113
protected

Definition at line 4590 of file NPSMEFTd6.h.

◆ CLQ3_3311

double NPSMEFTd6::CLQ3_3311
protected

Definition at line 4590 of file NPSMEFTd6.h.

◆ CLQ3_3323

double NPSMEFTd6::CLQ3_3323
protected

Definition at line 4591 of file NPSMEFTd6.h.

◆ CLQ3_3332

double NPSMEFTd6::CLQ3_3332
protected

Definition at line 4592 of file NPSMEFTd6.h.

◆ CLu_1111

double NPSMEFTd6::CLu_1111
protected

Definition at line 4608 of file NPSMEFTd6.h.

◆ CLu_1122

double NPSMEFTd6::CLu_1122
protected

Definition at line 4609 of file NPSMEFTd6.h.

◆ CLu_1133

double NPSMEFTd6::CLu_1133
protected

Definition at line 4610 of file NPSMEFTd6.h.

◆ CLu_2211

double NPSMEFTd6::CLu_2211
protected

Definition at line 4609 of file NPSMEFTd6.h.

◆ CLu_2233

double NPSMEFTd6::CLu_2233
protected

Definition at line 4611 of file NPSMEFTd6.h.

◆ CLu_3311

double NPSMEFTd6::CLu_3311
protected

Definition at line 4610 of file NPSMEFTd6.h.

◆ CpLedQ_11

double NPSMEFTd6::CpLedQ_11
protected

Definition at line 4622 of file NPSMEFTd6.h.

◆ CpLedQ_22

double NPSMEFTd6::CpLedQ_22
protected

Definition at line 4622 of file NPSMEFTd6.h.

◆ CQe_1111

double NPSMEFTd6::CQe_1111
protected

Definition at line 4617 of file NPSMEFTd6.h.

◆ CQe_1122

double NPSMEFTd6::CQe_1122
protected

Definition at line 4618 of file NPSMEFTd6.h.

◆ CQe_1133

double NPSMEFTd6::CQe_1133
protected

Definition at line 4619 of file NPSMEFTd6.h.

◆ CQe_2211

double NPSMEFTd6::CQe_2211
protected

Definition at line 4618 of file NPSMEFTd6.h.

◆ CQe_2311

double NPSMEFTd6::CQe_2311
protected

Definition at line 4620 of file NPSMEFTd6.h.

◆ CQe_2322

double NPSMEFTd6::CQe_2322
protected

Definition at line 4620 of file NPSMEFTd6.h.

◆ CQe_2333

double NPSMEFTd6::CQe_2333
protected

Definition at line 4620 of file NPSMEFTd6.h.

◆ CQe_3211

double NPSMEFTd6::CQe_3211
protected

Definition at line 4621 of file NPSMEFTd6.h.

◆ CQe_3222

double NPSMEFTd6::CQe_3222
protected

Definition at line 4621 of file NPSMEFTd6.h.

◆ CQe_3233

double NPSMEFTd6::CQe_3233
protected

Definition at line 4621 of file NPSMEFTd6.h.

◆ CQe_3311

double NPSMEFTd6::CQe_3311
protected

Definition at line 4619 of file NPSMEFTd6.h.

◆ CT

double NPSMEFTd6::CT
protected

The dimension-6 operator coefficient \(C_{T}\).

Definition at line 4430 of file NPSMEFTd6.h.

◆ CuB_11i

double NPSMEFTd6::CuB_11i
protected

The dimension-6 operator coefficient \((C_{uB})_{11}\) (imaginary part).

Definition at line 4574 of file NPSMEFTd6.h.

◆ CuB_11r

double NPSMEFTd6::CuB_11r
protected

The dimension-6 operator coefficient \((C_{uB})_{11}\) (real part).

Definition at line 4568 of file NPSMEFTd6.h.

◆ CuB_12i

double NPSMEFTd6::CuB_12i
protected

The dimension-6 operator coefficient \((C_{uB})_{12}\) (imaginary part).

Definition at line 4575 of file NPSMEFTd6.h.

◆ CuB_12r

double NPSMEFTd6::CuB_12r
protected

The dimension-6 operator coefficient \((C_{uB})_{12}\) (real part).

Definition at line 4569 of file NPSMEFTd6.h.

◆ CuB_13i

double NPSMEFTd6::CuB_13i
protected

The dimension-6 operator coefficient \((C_{uB})_{13}\) (imaginary part).

Definition at line 4576 of file NPSMEFTd6.h.

◆ CuB_13r

double NPSMEFTd6::CuB_13r
protected

The dimension-6 operator coefficient \((C_{uB})_{13}\) (real part).

Definition at line 4570 of file NPSMEFTd6.h.

◆ CuB_22i

double NPSMEFTd6::CuB_22i
protected

The dimension-6 operator coefficient \((C_{uB})_{22}\) (imaginary part).

Definition at line 4577 of file NPSMEFTd6.h.

◆ CuB_22r

double NPSMEFTd6::CuB_22r
protected

The dimension-6 operator coefficient \((C_{uB})_{22}\) (real part).

Definition at line 4571 of file NPSMEFTd6.h.

◆ CuB_23i

double NPSMEFTd6::CuB_23i
protected

The dimension-6 operator coefficient \((C_{uB})_{23}\) (imaginary part).

Definition at line 4578 of file NPSMEFTd6.h.

◆ CuB_23r

double NPSMEFTd6::CuB_23r
protected

The dimension-6 operator coefficient \((C_{uB})_{23}\) (real part).

Definition at line 4572 of file NPSMEFTd6.h.

◆ CuB_33i

double NPSMEFTd6::CuB_33i
protected

The dimension-6 operator coefficient \((C_{uB})_{33}\) (imaginary part).

Definition at line 4579 of file NPSMEFTd6.h.

◆ CuB_33r

double NPSMEFTd6::CuB_33r
protected

The dimension-6 operator coefficient \((C_{uB})_{33}\) (real part).

Definition at line 4573 of file NPSMEFTd6.h.

◆ CuG_11i

double NPSMEFTd6::CuG_11i
protected

The dimension-6 operator coefficient \((C_{uG})_{11}\) (imaginary part).

Definition at line 4550 of file NPSMEFTd6.h.

◆ CuG_11r

double NPSMEFTd6::CuG_11r
protected

The dimension-6 operator coefficient \((C_{uG})_{11}\) (real part).

Definition at line 4544 of file NPSMEFTd6.h.

◆ CuG_12i

double NPSMEFTd6::CuG_12i
protected

The dimension-6 operator coefficient \((C_{uG})_{12}\) (imaginary part).

Definition at line 4551 of file NPSMEFTd6.h.

◆ CuG_12r

double NPSMEFTd6::CuG_12r
protected

The dimension-6 operator coefficient \((C_{uG})_{12}\) (real part).

Definition at line 4545 of file NPSMEFTd6.h.

◆ CuG_13i

double NPSMEFTd6::CuG_13i
protected

The dimension-6 operator coefficient \((C_{uG})_{13}\) (imaginary part).

Definition at line 4552 of file NPSMEFTd6.h.

◆ CuG_13r

double NPSMEFTd6::CuG_13r
protected

The dimension-6 operator coefficient \((C_{uG})_{13}\) (real part).

Definition at line 4546 of file NPSMEFTd6.h.

◆ CuG_22i

double NPSMEFTd6::CuG_22i
protected

The dimension-6 operator coefficient \((C_{uG})_{22}\) (imaginary part).

Definition at line 4553 of file NPSMEFTd6.h.

◆ CuG_22r

double NPSMEFTd6::CuG_22r
protected

The dimension-6 operator coefficient \((C_{uG})_{22}\) (real part).

Definition at line 4547 of file NPSMEFTd6.h.

◆ CuG_23i

double NPSMEFTd6::CuG_23i
protected

The dimension-6 operator coefficient \((C_{uG})_{23}\) (imaginary part).

Definition at line 4554 of file NPSMEFTd6.h.

◆ CuG_23r

double NPSMEFTd6::CuG_23r
protected

The dimension-6 operator coefficient \((C_{uG})_{23}\) (real part).

Definition at line 4548 of file NPSMEFTd6.h.

◆ CuG_33i

double NPSMEFTd6::CuG_33i
protected

The dimension-6 operator coefficient \((C_{uG})_{33}\) (imaginary part).

Definition at line 4555 of file NPSMEFTd6.h.

◆ CuG_33r

double NPSMEFTd6::CuG_33r
protected

The dimension-6 operator coefficient \((C_{uG})_{33}\) (real part).

Definition at line 4549 of file NPSMEFTd6.h.

◆ CuH_11i

double NPSMEFTd6::CuH_11i
protected

The dimension-6 operator coefficient \((C_{uH})_{11}\) (imaginary part).

Definition at line 4526 of file NPSMEFTd6.h.

◆ CuH_11r

double NPSMEFTd6::CuH_11r
protected

The dimension-6 operator coefficient \((C_{uH})_{11}\) (real part).

Definition at line 4520 of file NPSMEFTd6.h.

◆ CuH_12i

double NPSMEFTd6::CuH_12i
protected

The dimension-6 operator coefficient \((C_{uH})_{12}\) (imaginary part).

Definition at line 4527 of file NPSMEFTd6.h.

◆ CuH_12r

double NPSMEFTd6::CuH_12r
protected

The dimension-6 operator coefficient \((C_{uH})_{12}\) (real part).

Definition at line 4521 of file NPSMEFTd6.h.

◆ CuH_13i

double NPSMEFTd6::CuH_13i
protected

The dimension-6 operator coefficient \((C_{uH})_{13}\) (imaginary part).

Definition at line 4528 of file NPSMEFTd6.h.

◆ CuH_13r

double NPSMEFTd6::CuH_13r
protected

The dimension-6 operator coefficient \((C_{uH})_{13}\) (real part).

Definition at line 4522 of file NPSMEFTd6.h.

◆ CuH_22i

double NPSMEFTd6::CuH_22i
protected

The dimension-6 operator coefficient \((C_{uH})_{22}\) (imaginary part).

Definition at line 4529 of file NPSMEFTd6.h.

◆ CuH_22r

double NPSMEFTd6::CuH_22r
protected

The dimension-6 operator coefficient \((C_{uH})_{22}\) (real part).

Definition at line 4523 of file NPSMEFTd6.h.

◆ CuH_23i

double NPSMEFTd6::CuH_23i
protected

The dimension-6 operator coefficient \((C_{uH})_{23}\) (imaginary part).

Definition at line 4530 of file NPSMEFTd6.h.

◆ CuH_23r

double NPSMEFTd6::CuH_23r
protected

The dimension-6 operator coefficient \((C_{uH})_{23}\) (real part).

Definition at line 4524 of file NPSMEFTd6.h.

◆ CuH_33i

double NPSMEFTd6::CuH_33i
protected

The dimension-6 operator coefficient \((C_{uH})_{33}\) (imaginary part).

Definition at line 4531 of file NPSMEFTd6.h.

◆ CuH_33r

double NPSMEFTd6::CuH_33r
protected

The dimension-6 operator coefficient \((C_{uH})_{33}\) (real part).

Definition at line 4525 of file NPSMEFTd6.h.

◆ CuW_11i

double NPSMEFTd6::CuW_11i
protected

The dimension-6 operator coefficient \((C_{uW})_{11}\) (imaginary part).

Definition at line 4562 of file NPSMEFTd6.h.

◆ CuW_11r

double NPSMEFTd6::CuW_11r
protected

The dimension-6 operator coefficient \((C_{uW})_{11}\) (real part).

Definition at line 4556 of file NPSMEFTd6.h.

◆ CuW_12i

double NPSMEFTd6::CuW_12i
protected

The dimension-6 operator coefficient \((C_{uW})_{12}\) (imaginary part).

Definition at line 4563 of file NPSMEFTd6.h.

◆ CuW_12r

double NPSMEFTd6::CuW_12r
protected

The dimension-6 operator coefficient \((C_{uW})_{12}\) (real part).

Definition at line 4557 of file NPSMEFTd6.h.

◆ CuW_13i

double NPSMEFTd6::CuW_13i
protected

The dimension-6 operator coefficient \((C_{uW})_{13}\) (imaginary part).

Definition at line 4564 of file NPSMEFTd6.h.

◆ CuW_13r

double NPSMEFTd6::CuW_13r
protected

The dimension-6 operator coefficient \((C_{uW})_{13}\) (real part).

Definition at line 4558 of file NPSMEFTd6.h.

◆ CuW_22i

double NPSMEFTd6::CuW_22i
protected

The dimension-6 operator coefficient \((C_{uW})_{22}\) (imaginary part).

Definition at line 4565 of file NPSMEFTd6.h.

◆ CuW_22r

double NPSMEFTd6::CuW_22r
protected

The dimension-6 operator coefficient \((C_{uW})_{22}\) (real part).

Definition at line 4559 of file NPSMEFTd6.h.

◆ CuW_23i

double NPSMEFTd6::CuW_23i
protected

The dimension-6 operator coefficient \((C_{uW})_{23}\) (imaginary part).

Definition at line 4566 of file NPSMEFTd6.h.

◆ CuW_23r

double NPSMEFTd6::CuW_23r
protected

The dimension-6 operator coefficient \((C_{uW})_{23}\) (real part).

Definition at line 4560 of file NPSMEFTd6.h.

◆ CuW_33i

double NPSMEFTd6::CuW_33i
protected

The dimension-6 operator coefficient \((C_{uW})_{33}\) (imaginary part).

Definition at line 4567 of file NPSMEFTd6.h.

◆ CuW_33r

double NPSMEFTd6::CuW_33r
protected

The dimension-6 operator coefficient \((C_{uW})_{33}\) (real part).

Definition at line 4561 of file NPSMEFTd6.h.

◆ CW

double NPSMEFTd6::CW
protected

The dimension-6 operator coefficient \(C_{W}\).

Definition at line 4414 of file NPSMEFTd6.h.

◆ cW2_tree

double NPSMEFTd6::cW2_tree
protected

The square of the tree level values for the cosine of the weak angle.

Definition at line 4880 of file NPSMEFTd6.h.

◆ cW_tree

double NPSMEFTd6::cW_tree
protected

The tree level values for the cosine of the weak angle.

Definition at line 4878 of file NPSMEFTd6.h.

◆ delta_AA

double NPSMEFTd6::delta_AA
protected

Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition.

Definition at line 4896 of file NPSMEFTd6.h.

◆ delta_AZ

double NPSMEFTd6::delta_AZ
protected

Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition.

Definition at line 4897 of file NPSMEFTd6.h.

◆ delta_h

double NPSMEFTd6::delta_h
protected

Combinations of dimension 6 coefficients modifying the \(H\) canonical field definition.

Definition at line 4898 of file NPSMEFTd6.h.

◆ delta_ZZ

double NPSMEFTd6::delta_ZZ
protected

Combination of dimension 6 coefficients modifying the \(Z_\mu\) canonical field definition.

Definition at line 4895 of file NPSMEFTd6.h.

◆ dg1Z

double NPSMEFTd6::dg1Z
protected

Independent contribution to aTGC.

Definition at line 4797 of file NPSMEFTd6.h.

◆ dGammaHTotR1

double NPSMEFTd6::dGammaHTotR1
protected

Definition at line 4922 of file NPSMEFTd6.h.

◆ dGammaHTotR2

double NPSMEFTd6::dGammaHTotR2
protected

Definition at line 4922 of file NPSMEFTd6.h.

◆ dKappaga

double NPSMEFTd6::dKappaga
protected

Independent contribution to aTGC.

Definition at line 4798 of file NPSMEFTd6.h.

◆ dZH

double NPSMEFTd6::dZH
protected

Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.

Definition at line 4902 of file NPSMEFTd6.h.

◆ eeettHint

double NPSMEFTd6::eeettHint
protected

Intrinsic relative theoretical error in \(e^+ e^- \to t \bar{t} H\). (Assumed to be constant in energy.)

Definition at line 4639 of file NPSMEFTd6.h.

◆ eeettHpar

double NPSMEFTd6::eeettHpar
protected

Parametric relative theoretical error in \(e^+ e^- \to t \bar{t} H\). (Assumed to be constant in energy.)

Definition at line 4640 of file NPSMEFTd6.h.

◆ eeeWBFint

double NPSMEFTd6::eeeWBFint
protected

Intrinsic relative theoretical error in \(e^+ e^- \to H \bar{\nu} \nu\). (Assumed to be constant in energy.)

Definition at line 4635 of file NPSMEFTd6.h.

◆ eeeWBFpar

double NPSMEFTd6::eeeWBFpar
protected

Parametric relative theoretical error in \(e^+ e^- \to H \bar{\nu} \nu\). (Assumed to be constant in energy.)

Definition at line 4636 of file NPSMEFTd6.h.

◆ eeeZHint

double NPSMEFTd6::eeeZHint
protected

Intrinsic relative theoretical error in \(e^+ e^- \to Z H\). (Assumed to be constant in energy.)

Definition at line 4637 of file NPSMEFTd6.h.

◆ eeeZHpar

double NPSMEFTd6::eeeZHpar
protected

Parametric relative theoretical error in \(e^+ e^- \to Z H\). (Assumed to be constant in energy.)

Definition at line 4638 of file NPSMEFTd6.h.

◆ eeMz

double NPSMEFTd6::eeMz
protected

The em coupling at Mz.

Definition at line 4876 of file NPSMEFTd6.h.

◆ eeMz2

double NPSMEFTd6::eeMz2
protected

The em coupling squared (at Mz).

Definition at line 4877 of file NPSMEFTd6.h.

◆ eepWBFint

double NPSMEFTd6::eepWBFint
protected

Intrinsic relative theoretical error in \(e^- p \to H e^- j\) via WBF. (Assumed to be constant in energy.)

Definition at line 4641 of file NPSMEFTd6.h.

◆ eepWBFpar

double NPSMEFTd6::eepWBFpar
protected

Parametric relative theoretical error in \(e^- p \to H e^- j\) via WBF. (Assumed to be constant in energy.)

Definition at line 4642 of file NPSMEFTd6.h.

◆ eepZBFint

double NPSMEFTd6::eepZBFint
protected

Intrinsic relative theoretical error in \(e^- p \to H e^- j\) via ZBF. (Assumed to be constant in energy.)

Definition at line 4643 of file NPSMEFTd6.h.

◆ eepZBFpar

double NPSMEFTd6::eepZBFpar
protected

Parametric relative theoretical error in \(e^- p \to H e^- j\) via ZBF. (Assumed to be constant in energy.)

Definition at line 4644 of file NPSMEFTd6.h.

◆ eggFHbb

double NPSMEFTd6::eggFHbb
protected

Definition at line 4664 of file NPSMEFTd6.h.

◆ eggFHgaga

double NPSMEFTd6::eggFHgaga
protected

Definition at line 4664 of file NPSMEFTd6.h.

◆ eggFHmumu

double NPSMEFTd6::eggFHmumu
protected

Total relative theoretical error in \(gg \to H \to X\).

Definition at line 4664 of file NPSMEFTd6.h.

◆ eggFHtautau

double NPSMEFTd6::eggFHtautau
protected

Definition at line 4664 of file NPSMEFTd6.h.

◆ eggFHWW

double NPSMEFTd6::eggFHWW
protected

Definition at line 4664 of file NPSMEFTd6.h.

◆ eggFHZga

double NPSMEFTd6::eggFHZga
protected

Definition at line 4664 of file NPSMEFTd6.h.

◆ eggFHZZ

double NPSMEFTd6::eggFHZZ
protected

Definition at line 4664 of file NPSMEFTd6.h.

◆ eggFint

double NPSMEFTd6::eggFint
protected

Intrinsic relative theoretical error in ggF production. (Assumed to be constant in energy.)

Definition at line 4625 of file NPSMEFTd6.h.

◆ eggFpar

double NPSMEFTd6::eggFpar
protected

Parametric relative theoretical error in ggF production. (Assumed to be constant in energy.)

Definition at line 4626 of file NPSMEFTd6.h.

◆ eHbbint

double NPSMEFTd6::eHbbint
protected

Intrinsic relative theoretical error in \(H \to b\bar{b}\).

Definition at line 4661 of file NPSMEFTd6.h.

◆ eHbbpar

double NPSMEFTd6::eHbbpar
protected

Parametric relative theoretical error in \(H \to b\bar{b}\).

Definition at line 4662 of file NPSMEFTd6.h.

◆ eHccint

double NPSMEFTd6::eHccint
protected

Intrinsic relative theoretical error in \(H \to c\bar{c}\).

Definition at line 4659 of file NPSMEFTd6.h.

◆ eHccpar

double NPSMEFTd6::eHccpar
protected

Parametric relative theoretical error in \(H \to c\bar{c}\).

Definition at line 4660 of file NPSMEFTd6.h.

◆ eHgagaint

double NPSMEFTd6::eHgagaint
protected

Intrinsic relative theoretical error in \(H \to \gamma\gamma\).

Definition at line 4653 of file NPSMEFTd6.h.

◆ eHgagapar

double NPSMEFTd6::eHgagapar
protected

Parametric relative theoretical error in \(H \to \gamma\gamma\).

Definition at line 4654 of file NPSMEFTd6.h.

◆ eHggint

double NPSMEFTd6::eHggint
protected

Intrinsic relative theoretical error in \(H \to g g\).

Definition at line 4645 of file NPSMEFTd6.h.

◆ eHggpar

double NPSMEFTd6::eHggpar
protected

Parametric relative theoretical error in \(H \to g g\).

Definition at line 4646 of file NPSMEFTd6.h.

◆ eHmumuint

double NPSMEFTd6::eHmumuint
protected

Intrinsic relative theoretical error in \(H \to \mu^+ \mu^-\).

Definition at line 4655 of file NPSMEFTd6.h.

◆ eHmumupar

double NPSMEFTd6::eHmumupar
protected

Parametric relative theoretical error in \(H \to \mu^+ \mu^-\).

Definition at line 4656 of file NPSMEFTd6.h.

◆ eHtautauint

double NPSMEFTd6::eHtautauint
protected

Intrinsic relative theoretical error in \(H \to \tau^+ \tau^-\).

Definition at line 4657 of file NPSMEFTd6.h.

◆ eHtautaupar

double NPSMEFTd6::eHtautaupar
protected

Parametric relative theoretical error in \(H \to \tau^+ \tau^-\).

Definition at line 4658 of file NPSMEFTd6.h.

◆ eHwidth

double NPSMEFTd6::eHwidth
protected

Total relative theoretical error in the Higgs width.

Definition at line 4671 of file NPSMEFTd6.h.

◆ eHWWint

double NPSMEFTd6::eHWWint
protected

Intrinsic relative theoretical error in \(H \to W W\).

Definition at line 4647 of file NPSMEFTd6.h.

◆ eHWWpar

double NPSMEFTd6::eHWWpar
protected

Parametric relative theoretical error in \(H \to W W\).

Definition at line 4648 of file NPSMEFTd6.h.

◆ eHZgaint

double NPSMEFTd6::eHZgaint
protected

Intrinsic relative theoretical error in \(H \to Z \gamma\).

Definition at line 4651 of file NPSMEFTd6.h.

◆ eHZgapar

double NPSMEFTd6::eHZgapar
protected

Parametric relative theoretical error in \(H \to Z \gamma\).

Definition at line 4652 of file NPSMEFTd6.h.

◆ eHZZint

double NPSMEFTd6::eHZZint
protected

Intrinsic relative theoretical error in \(H \to Z Z\).

Definition at line 4649 of file NPSMEFTd6.h.

◆ eHZZpar

double NPSMEFTd6::eHZZpar
protected

Parametric relative theoretical error in \(H \to Z Z\).

Definition at line 4650 of file NPSMEFTd6.h.

◆ ettH_1314_DeltagHt

double NPSMEFTd6::ettH_1314_DeltagHt
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (13 & 14 TeV).

Definition at line 4792 of file NPSMEFTd6.h.

◆ ettH_1314_G

double NPSMEFTd6::ettH_1314_G
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (13 & 14 TeV).

Definition at line 4790 of file NPSMEFTd6.h.

◆ ettH_1314_HG

double NPSMEFTd6::ettH_1314_HG
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (13 & 14 TeV).

Definition at line 4789 of file NPSMEFTd6.h.

◆ ettH_1314_uG_33r

double NPSMEFTd6::ettH_1314_uG_33r
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (13 & 14 TeV).

Definition at line 4791 of file NPSMEFTd6.h.

◆ ettH_2_DeltagHt

double NPSMEFTd6::ettH_2_DeltagHt
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (1.96 TeV).

Definition at line 4782 of file NPSMEFTd6.h.

◆ ettH_2_G

double NPSMEFTd6::ettH_2_G
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (1.96 TeV).

Definition at line 4780 of file NPSMEFTd6.h.

◆ ettH_2_HG

double NPSMEFTd6::ettH_2_HG
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (1.96 TeV).

Definition at line 4779 of file NPSMEFTd6.h.

◆ ettH_2_uG_33r

double NPSMEFTd6::ettH_2_uG_33r
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (1.96 TeV).

Definition at line 4781 of file NPSMEFTd6.h.

◆ ettH_78_DeltagHt

double NPSMEFTd6::ettH_78_DeltagHt
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (7 & 8 TeV).

Definition at line 4787 of file NPSMEFTd6.h.

◆ ettH_78_G

double NPSMEFTd6::ettH_78_G
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (7 & 8 TeV).

Definition at line 4785 of file NPSMEFTd6.h.

◆ ettH_78_HG

double NPSMEFTd6::ettH_78_HG
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (7 & 8 TeV).

Definition at line 4784 of file NPSMEFTd6.h.

◆ ettH_78_uG_33r

double NPSMEFTd6::ettH_78_uG_33r
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (7 & 8 TeV).

Definition at line 4786 of file NPSMEFTd6.h.

◆ ettHbb

double NPSMEFTd6::ettHbb
protected

Definition at line 4668 of file NPSMEFTd6.h.

◆ ettHgaga

double NPSMEFTd6::ettHgaga
protected

Definition at line 4668 of file NPSMEFTd6.h.

◆ ettHint

double NPSMEFTd6::ettHint
protected

Intrinsic relative theoretical error in ttH production. (Assumed to be constant in energy.)

Definition at line 4627 of file NPSMEFTd6.h.

◆ ettHmumu

double NPSMEFTd6::ettHmumu
protected

Total relative theoretical error in \(pp \to ttH \to tt X\).

Definition at line 4668 of file NPSMEFTd6.h.

◆ ettHpar

double NPSMEFTd6::ettHpar
protected

Parametric relative theoretical error in ttH production. (Assumed to be constant in energy.)

Definition at line 4628 of file NPSMEFTd6.h.

◆ ettHtautau

double NPSMEFTd6::ettHtautau
protected

Definition at line 4668 of file NPSMEFTd6.h.

◆ ettHWW

double NPSMEFTd6::ettHWW
protected

Definition at line 4668 of file NPSMEFTd6.h.

◆ ettHZga

double NPSMEFTd6::ettHZga
protected

Definition at line 4668 of file NPSMEFTd6.h.

◆ ettHZZ

double NPSMEFTd6::ettHZZ
protected

Definition at line 4668 of file NPSMEFTd6.h.

◆ eVBF_1314_DeltaGF

double NPSMEFTd6::eVBF_1314_DeltaGF
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 4714 of file NPSMEFTd6.h.

◆ eVBF_1314_DHB

double NPSMEFTd6::eVBF_1314_DHB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 4712 of file NPSMEFTd6.h.

◆ eVBF_1314_DHW

double NPSMEFTd6::eVBF_1314_DHW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 4713 of file NPSMEFTd6.h.

◆ eVBF_1314_HB

double NPSMEFTd6::eVBF_1314_HB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 4708 of file NPSMEFTd6.h.

◆ eVBF_1314_Hbox

double NPSMEFTd6::eVBF_1314_Hbox
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 4702 of file NPSMEFTd6.h.

◆ eVBF_1314_HD

double NPSMEFTd6::eVBF_1314_HD
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 4707 of file NPSMEFTd6.h.

◆ eVBF_1314_Hd_11

double NPSMEFTd6::eVBF_1314_Hd_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 4705 of file NPSMEFTd6.h.

◆ eVBF_1314_HG

double NPSMEFTd6::eVBF_1314_HG
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 4711 of file NPSMEFTd6.h.

◆ eVBF_1314_HQ1_11

double NPSMEFTd6::eVBF_1314_HQ1_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 4703 of file NPSMEFTd6.h.

◆ eVBF_1314_HQ3_11

double NPSMEFTd6::eVBF_1314_HQ3_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 4706 of file NPSMEFTd6.h.

◆ eVBF_1314_Hu_11

double NPSMEFTd6::eVBF_1314_Hu_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 4704 of file NPSMEFTd6.h.

◆ eVBF_1314_HW

double NPSMEFTd6::eVBF_1314_HW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 4709 of file NPSMEFTd6.h.

◆ eVBF_1314_HWB

double NPSMEFTd6::eVBF_1314_HWB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 4710 of file NPSMEFTd6.h.

◆ eVBF_2_DeltaGF

double NPSMEFTd6::eVBF_2_DeltaGF
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 4686 of file NPSMEFTd6.h.

◆ eVBF_2_DHB

double NPSMEFTd6::eVBF_2_DHB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 4684 of file NPSMEFTd6.h.

◆ eVBF_2_DHW

double NPSMEFTd6::eVBF_2_DHW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 4685 of file NPSMEFTd6.h.

◆ eVBF_2_HB

double NPSMEFTd6::eVBF_2_HB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 4680 of file NPSMEFTd6.h.

◆ eVBF_2_Hbox

double NPSMEFTd6::eVBF_2_Hbox
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 4674 of file NPSMEFTd6.h.

◆ eVBF_2_HD

double NPSMEFTd6::eVBF_2_HD
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 4679 of file NPSMEFTd6.h.

◆ eVBF_2_Hd_11

double NPSMEFTd6::eVBF_2_Hd_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 4677 of file NPSMEFTd6.h.

◆ eVBF_2_HG

double NPSMEFTd6::eVBF_2_HG
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 4683 of file NPSMEFTd6.h.

◆ eVBF_2_HQ1_11

double NPSMEFTd6::eVBF_2_HQ1_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 4675 of file NPSMEFTd6.h.

◆ eVBF_2_HQ3_11

double NPSMEFTd6::eVBF_2_HQ3_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 4678 of file NPSMEFTd6.h.

◆ eVBF_2_Hu_11

double NPSMEFTd6::eVBF_2_Hu_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 4676 of file NPSMEFTd6.h.

◆ eVBF_2_HW

double NPSMEFTd6::eVBF_2_HW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 4681 of file NPSMEFTd6.h.

◆ eVBF_2_HWB

double NPSMEFTd6::eVBF_2_HWB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 4682 of file NPSMEFTd6.h.

◆ eVBF_78_DeltaGF

double NPSMEFTd6::eVBF_78_DeltaGF
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 4700 of file NPSMEFTd6.h.

◆ eVBF_78_DHB

double NPSMEFTd6::eVBF_78_DHB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 4698 of file NPSMEFTd6.h.

◆ eVBF_78_DHW

double NPSMEFTd6::eVBF_78_DHW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 4699 of file NPSMEFTd6.h.

◆ eVBF_78_HB

double NPSMEFTd6::eVBF_78_HB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 4694 of file NPSMEFTd6.h.

◆ eVBF_78_Hbox

double NPSMEFTd6::eVBF_78_Hbox
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 4688 of file NPSMEFTd6.h.

◆ eVBF_78_HD

double NPSMEFTd6::eVBF_78_HD
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 4693 of file NPSMEFTd6.h.

◆ eVBF_78_Hd_11

double NPSMEFTd6::eVBF_78_Hd_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 4691 of file NPSMEFTd6.h.

◆ eVBF_78_HG

double NPSMEFTd6::eVBF_78_HG
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 4697 of file NPSMEFTd6.h.

◆ eVBF_78_HQ1_11

double NPSMEFTd6::eVBF_78_HQ1_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 4689 of file NPSMEFTd6.h.

◆ eVBF_78_HQ3_11

double NPSMEFTd6::eVBF_78_HQ3_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 4692 of file NPSMEFTd6.h.

◆ eVBF_78_Hu_11

double NPSMEFTd6::eVBF_78_Hu_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 4690 of file NPSMEFTd6.h.

◆ eVBF_78_HW

double NPSMEFTd6::eVBF_78_HW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 4695 of file NPSMEFTd6.h.

◆ eVBF_78_HWB

double NPSMEFTd6::eVBF_78_HWB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 4696 of file NPSMEFTd6.h.

◆ eVBFHbb

double NPSMEFTd6::eVBFHbb
protected

Definition at line 4665 of file NPSMEFTd6.h.

◆ eVBFHgaga

double NPSMEFTd6::eVBFHgaga
protected

Definition at line 4665 of file NPSMEFTd6.h.

◆ eVBFHinv

double NPSMEFTd6::eVBFHinv
protected

Definition at line 4669 of file NPSMEFTd6.h.

◆ eVBFHmumu

double NPSMEFTd6::eVBFHmumu
protected

Total relative theoretical error in \(pp \to Hjj (VBF) \to X jj\).

Definition at line 4665 of file NPSMEFTd6.h.

◆ eVBFHtautau

double NPSMEFTd6::eVBFHtautau
protected

Definition at line 4665 of file NPSMEFTd6.h.

◆ eVBFHWW

double NPSMEFTd6::eVBFHWW
protected

Definition at line 4665 of file NPSMEFTd6.h.

◆ eVBFHZga

double NPSMEFTd6::eVBFHZga
protected

Definition at line 4665 of file NPSMEFTd6.h.

◆ eVBFHZZ

double NPSMEFTd6::eVBFHZZ
protected

Definition at line 4665 of file NPSMEFTd6.h.

◆ eVBFint

double NPSMEFTd6::eVBFint
protected

Intrinsic relative theoretical error in VBF production. (Assumed to be constant in energy.)

Definition at line 4629 of file NPSMEFTd6.h.

◆ eVBFpar

double NPSMEFTd6::eVBFpar
protected

Parametric relative theoretical error in VBF production. (Assumed to be constant in energy.)

Definition at line 4630 of file NPSMEFTd6.h.

◆ eVHinv

double NPSMEFTd6::eVHinv
protected

Total relative theoretical error in \(pp \to X H \to X + invisible\).

Definition at line 4669 of file NPSMEFTd6.h.

◆ eWH_1314_DeltaGF

double NPSMEFTd6::eWH_1314_DeltaGF
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (13 & 14 TeV).

Definition at line 4738 of file NPSMEFTd6.h.

◆ eWH_1314_DHW

double NPSMEFTd6::eWH_1314_DHW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (13 & 14 TeV).

Definition at line 4737 of file NPSMEFTd6.h.

◆ eWH_1314_Hbox

double NPSMEFTd6::eWH_1314_Hbox
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (13 & 14 TeV).

Definition at line 4732 of file NPSMEFTd6.h.

◆ eWH_1314_HD

double NPSMEFTd6::eWH_1314_HD
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (13 & 14 TeV).

Definition at line 4734 of file NPSMEFTd6.h.

◆ eWH_1314_HQ3_11

double NPSMEFTd6::eWH_1314_HQ3_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (13 & 14 TeV).

Definition at line 4733 of file NPSMEFTd6.h.

◆ eWH_1314_HW

double NPSMEFTd6::eWH_1314_HW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (13 & 14 TeV).

Definition at line 4735 of file NPSMEFTd6.h.

◆ eWH_1314_HWB

double NPSMEFTd6::eWH_1314_HWB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (13 & 14 TeV).

Definition at line 4736 of file NPSMEFTd6.h.

◆ eWH_2_DeltaGF

double NPSMEFTd6::eWH_2_DeltaGF
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (1.96 TeV).

Definition at line 4722 of file NPSMEFTd6.h.

◆ eWH_2_DHW

double NPSMEFTd6::eWH_2_DHW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (1.96 TeV).

Definition at line 4721 of file NPSMEFTd6.h.

◆ eWH_2_Hbox

double NPSMEFTd6::eWH_2_Hbox
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (1.96 TeV).

Definition at line 4716 of file NPSMEFTd6.h.

◆ eWH_2_HD

double NPSMEFTd6::eWH_2_HD
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (1.96 TeV).

Definition at line 4718 of file NPSMEFTd6.h.

◆ eWH_2_HQ3_11

double NPSMEFTd6::eWH_2_HQ3_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (1.96 TeV).

Definition at line 4717 of file NPSMEFTd6.h.

◆ eWH_2_HW

double NPSMEFTd6::eWH_2_HW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (1.96 TeV).

Definition at line 4719 of file NPSMEFTd6.h.

◆ eWH_2_HWB

double NPSMEFTd6::eWH_2_HWB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (1.96 TeV).

Definition at line 4720 of file NPSMEFTd6.h.

◆ eWH_78_DeltaGF

double NPSMEFTd6::eWH_78_DeltaGF
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (7 & 8 TeV).

Definition at line 4730 of file NPSMEFTd6.h.

◆ eWH_78_DHW

double NPSMEFTd6::eWH_78_DHW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (7 & 8 TeV).

Definition at line 4729 of file NPSMEFTd6.h.

◆ eWH_78_Hbox

double NPSMEFTd6::eWH_78_Hbox
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (7 & 8 TeV).

Definition at line 4724 of file NPSMEFTd6.h.

◆ eWH_78_HD

double NPSMEFTd6::eWH_78_HD
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (7 & 8 TeV).

Definition at line 4726 of file NPSMEFTd6.h.

◆ eWH_78_HQ3_11

double NPSMEFTd6::eWH_78_HQ3_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (7 & 8 TeV).

Definition at line 4725 of file NPSMEFTd6.h.

◆ eWH_78_HW

double NPSMEFTd6::eWH_78_HW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (7 & 8 TeV).

Definition at line 4727 of file NPSMEFTd6.h.

◆ eWH_78_HWB

double NPSMEFTd6::eWH_78_HWB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (7 & 8 TeV).

Definition at line 4728 of file NPSMEFTd6.h.

◆ eWHbb

double NPSMEFTd6::eWHbb
protected

Definition at line 4666 of file NPSMEFTd6.h.

◆ eWHgaga

double NPSMEFTd6::eWHgaga
protected

Definition at line 4666 of file NPSMEFTd6.h.

◆ eWHint

double NPSMEFTd6::eWHint
protected

Intrinsic relative theoretical error in WH production. (Assumed to be constant in energy.)

Definition at line 4631 of file NPSMEFTd6.h.

◆ eWHmumu

double NPSMEFTd6::eWHmumu
protected

Total relative theoretical error in \(pp \to WH \to W X\).

Definition at line 4666 of file NPSMEFTd6.h.

◆ eWHpar

double NPSMEFTd6::eWHpar
protected

Parametric relative theoretical error in WH production. (Assumed to be constant in energy.)

Definition at line 4632 of file NPSMEFTd6.h.

◆ eWHtautau

double NPSMEFTd6::eWHtautau
protected

Definition at line 4666 of file NPSMEFTd6.h.

◆ eWHWW

double NPSMEFTd6::eWHWW
protected

Definition at line 4666 of file NPSMEFTd6.h.

◆ eWHZga

double NPSMEFTd6::eWHZga
protected

Definition at line 4666 of file NPSMEFTd6.h.

◆ eWHZZ

double NPSMEFTd6::eWHZZ
protected

Definition at line 4666 of file NPSMEFTd6.h.

◆ eZH_1314_DeltaGF

double NPSMEFTd6::eZH_1314_DeltaGF
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 4777 of file NPSMEFTd6.h.

◆ eZH_1314_DHB

double NPSMEFTd6::eZH_1314_DHB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 4775 of file NPSMEFTd6.h.

◆ eZH_1314_DHW

double NPSMEFTd6::eZH_1314_DHW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 4776 of file NPSMEFTd6.h.

◆ eZH_1314_HB

double NPSMEFTd6::eZH_1314_HB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 4772 of file NPSMEFTd6.h.

◆ eZH_1314_Hbox

double NPSMEFTd6::eZH_1314_Hbox
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 4766 of file NPSMEFTd6.h.

◆ eZH_1314_HD

double NPSMEFTd6::eZH_1314_HD
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 4771 of file NPSMEFTd6.h.

◆ eZH_1314_Hd_11

double NPSMEFTd6::eZH_1314_Hd_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 4769 of file NPSMEFTd6.h.

◆ eZH_1314_HQ1_11

double NPSMEFTd6::eZH_1314_HQ1_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 4767 of file NPSMEFTd6.h.

◆ eZH_1314_HQ3_11

double NPSMEFTd6::eZH_1314_HQ3_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 4770 of file NPSMEFTd6.h.

◆ eZH_1314_Hu_11

double NPSMEFTd6::eZH_1314_Hu_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 4768 of file NPSMEFTd6.h.

◆ eZH_1314_HW

double NPSMEFTd6::eZH_1314_HW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 4773 of file NPSMEFTd6.h.

◆ eZH_1314_HWB

double NPSMEFTd6::eZH_1314_HWB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 4774 of file NPSMEFTd6.h.

◆ eZH_2_DeltaGF

double NPSMEFTd6::eZH_2_DeltaGF
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 4751 of file NPSMEFTd6.h.

◆ eZH_2_DHB

double NPSMEFTd6::eZH_2_DHB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 4749 of file NPSMEFTd6.h.

◆ eZH_2_DHW

double NPSMEFTd6::eZH_2_DHW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 4750 of file NPSMEFTd6.h.

◆ eZH_2_HB

double NPSMEFTd6::eZH_2_HB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 4746 of file NPSMEFTd6.h.

◆ eZH_2_Hbox

double NPSMEFTd6::eZH_2_Hbox
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 4740 of file NPSMEFTd6.h.

◆ eZH_2_HD

double NPSMEFTd6::eZH_2_HD
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 4745 of file NPSMEFTd6.h.

◆ eZH_2_Hd_11

double NPSMEFTd6::eZH_2_Hd_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 4743 of file NPSMEFTd6.h.

◆ eZH_2_HQ1_11

double NPSMEFTd6::eZH_2_HQ1_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 4741 of file NPSMEFTd6.h.

◆ eZH_2_HQ3_11

double NPSMEFTd6::eZH_2_HQ3_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 4744 of file NPSMEFTd6.h.

◆ eZH_2_Hu_11

double NPSMEFTd6::eZH_2_Hu_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 4742 of file NPSMEFTd6.h.

◆ eZH_2_HW

double NPSMEFTd6::eZH_2_HW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 4747 of file NPSMEFTd6.h.

◆ eZH_2_HWB

double NPSMEFTd6::eZH_2_HWB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 4748 of file NPSMEFTd6.h.

◆ eZH_78_DeltaGF

double NPSMEFTd6::eZH_78_DeltaGF
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 4764 of file NPSMEFTd6.h.

◆ eZH_78_DHB

double NPSMEFTd6::eZH_78_DHB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 4762 of file NPSMEFTd6.h.

◆ eZH_78_DHW

double NPSMEFTd6::eZH_78_DHW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 4763 of file NPSMEFTd6.h.

◆ eZH_78_HB

double NPSMEFTd6::eZH_78_HB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 4759 of file NPSMEFTd6.h.

◆ eZH_78_Hbox

double NPSMEFTd6::eZH_78_Hbox
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 4753 of file NPSMEFTd6.h.

◆ eZH_78_HD

double NPSMEFTd6::eZH_78_HD
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 4758 of file NPSMEFTd6.h.

◆ eZH_78_Hd_11

double NPSMEFTd6::eZH_78_Hd_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 4756 of file NPSMEFTd6.h.

◆ eZH_78_HQ1_11

double NPSMEFTd6::eZH_78_HQ1_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 4754 of file NPSMEFTd6.h.

◆ eZH_78_HQ3_11

double NPSMEFTd6::eZH_78_HQ3_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 4757 of file NPSMEFTd6.h.

◆ eZH_78_Hu_11

double NPSMEFTd6::eZH_78_Hu_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 4755 of file NPSMEFTd6.h.

◆ eZH_78_HW

double NPSMEFTd6::eZH_78_HW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 4760 of file NPSMEFTd6.h.

◆ eZH_78_HWB

double NPSMEFTd6::eZH_78_HWB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 4761 of file NPSMEFTd6.h.

◆ eZHbb

double NPSMEFTd6::eZHbb
protected

Definition at line 4667 of file NPSMEFTd6.h.

◆ eZHgaga

double NPSMEFTd6::eZHgaga
protected

Definition at line 4667 of file NPSMEFTd6.h.

◆ eZHint

double NPSMEFTd6::eZHint
protected

Intrinsic relative theoretical error in ZH production. (Assumed to be constant in energy.)

Definition at line 4633 of file NPSMEFTd6.h.

◆ eZHmumu

double NPSMEFTd6::eZHmumu
protected

Total relative theoretical error in \(pp \to ZH \to Z X\).

Definition at line 4667 of file NPSMEFTd6.h.

◆ eZHpar

double NPSMEFTd6::eZHpar
protected

Parametric relative theoretical error in ZH production. (Assumed to be constant in energy.)

Definition at line 4634 of file NPSMEFTd6.h.

◆ eZHtautau

double NPSMEFTd6::eZHtautau
protected

Definition at line 4667 of file NPSMEFTd6.h.

◆ eZHWW

double NPSMEFTd6::eZHWW
protected

Definition at line 4667 of file NPSMEFTd6.h.

◆ eZHZga

double NPSMEFTd6::eZHZga
protected

Definition at line 4667 of file NPSMEFTd6.h.

◆ eZHZZ

double NPSMEFTd6::eZHZZ
protected

Definition at line 4667 of file NPSMEFTd6.h.

◆ FlagFlavU3OfX

bool NPSMEFTd6::FlagFlavU3OfX
private

A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients.

Definition at line 4987 of file NPSMEFTd6.h.

◆ FlagHiggsSM

bool NPSMEFTd6::FlagHiggsSM
private

A boolean flag that is true if including dependence on small variations of the SM parameters (dependence is linearized). Available only in selected Higgs observables.

Definition at line 4989 of file NPSMEFTd6.h.

◆ FlagLeptonUniversal

const bool NPSMEFTd6::FlagLeptonUniversal
private

An internal boolean flag that is true if assuming lepton flavour universality.

Definition at line 4997 of file NPSMEFTd6.h.

◆ FlagLoopH3d6Quad

bool NPSMEFTd6::FlagLoopH3d6Quad
private

A boolean flag that is true if including quadratic modifications in the SM loops in Higgs observables due to the dim 6 interactions that contribute to the trilinear Higgs coupling.

Definition at line 4991 of file NPSMEFTd6.h.

◆ FlagLoopHd6

bool NPSMEFTd6::FlagLoopHd6
private

A boolean flag that is true if including modifications in the SM loops in Higgs observables due to the dim 6 interactions.

Definition at line 4990 of file NPSMEFTd6.h.

◆ FlagPartialQFU

bool NPSMEFTd6::FlagPartialQFU
private

A boolean flag that is true if assuming partial quark flavour universality between the 1st and 2nd family in the CHF operators.

Definition at line 4986 of file NPSMEFTd6.h.

◆ FlagQuadraticTerms

bool NPSMEFTd6::FlagQuadraticTerms
private

A boolean flag that is true if the quadratic terms in cross sections and widths are switched on.

Definition at line 4984 of file NPSMEFTd6.h.

◆ FlagQuarkUniversal

const bool NPSMEFTd6::FlagQuarkUniversal
private

An internal boolean flag that is true if assuming quark flavour universality.

Definition at line 5003 of file NPSMEFTd6.h.

◆ FlagRotateCHWCHB

bool NPSMEFTd6::FlagRotateCHWCHB
private

A boolean flag that is true if we use as parameters CHWHB_gaga and CHWHB_gagaorth instead of CHW and CHB.

Definition at line 4985 of file NPSMEFTd6.h.

◆ FlagUnivOfX

bool NPSMEFTd6::FlagUnivOfX
private

A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients and all proportional to the same coefficient (CuH_33 and CuV_33 respectively).

Definition at line 4988 of file NPSMEFTd6.h.

◆ g1_tree

double NPSMEFTd6::g1_tree
protected

The tree level value of the \(U(1)_Y\) gauge coupling contant (at the \(Z\) pole).

Definition at line 4883 of file NPSMEFTd6.h.

◆ g2_tree

double NPSMEFTd6::g2_tree
protected

The tree level value of the \(SU(2)_L\) gauge coupling contant (at the \(Z\) pole).

Definition at line 4884 of file NPSMEFTd6.h.

◆ g3_tree

double NPSMEFTd6::g3_tree
protected

The tree level value of the \(SU(3)_c\) gauge coupling contant (at the \(Z\) pole).

Definition at line 4885 of file NPSMEFTd6.h.

◆ GammaHTotR

double NPSMEFTd6::GammaHTotR
protected

NP contributions and Total to Higgs width ratio with SM.

Definition at line 4922 of file NPSMEFTd6.h.

◆ gZdL

double NPSMEFTd6::gZdL
protected

Definition at line 4890 of file NPSMEFTd6.h.

◆ gZdR

double NPSMEFTd6::gZdR
protected

The tree level value of the \(Z\bar{d}d\) couplings in the SM.

Definition at line 4890 of file NPSMEFTd6.h.

◆ gZlL

double NPSMEFTd6::gZlL
protected

Definition at line 4888 of file NPSMEFTd6.h.

◆ gZlR

double NPSMEFTd6::gZlR
protected

The tree level value of the \(Z\ell^+\ell^-\) couplings in the SM.

Definition at line 4888 of file NPSMEFTd6.h.

◆ gZuL

double NPSMEFTd6::gZuL
protected

Definition at line 4889 of file NPSMEFTd6.h.

◆ gZuR

double NPSMEFTd6::gZuR
protected

The tree level value of the \(Z\bar{u}u\) couplings in the SM.

Definition at line 4889 of file NPSMEFTd6.h.

◆ gZvL

double NPSMEFTd6::gZvL
protected

The tree level value of the \(Z\bar{\nu}\nu\) couplings in the SM.

Definition at line 4887 of file NPSMEFTd6.h.

◆ Lambda_NP

double NPSMEFTd6::Lambda_NP
protected

The new physics scale [GeV].

Definition at line 4623 of file NPSMEFTd6.h.

◆ lambdaH_tree

double NPSMEFTd6::lambdaH_tree
protected

The SM tree level value of the scalar quartic coupling in the potential.

Definition at line 4900 of file NPSMEFTd6.h.

◆ LambdaNP2

double NPSMEFTd6::LambdaNP2
protected

The square of the new physics scale [GeV \(^2\)].

Definition at line 4805 of file NPSMEFTd6.h.

◆ lambZ

double NPSMEFTd6::lambZ
protected

Independent contribution to aTGC.

Definition at line 4799 of file NPSMEFTd6.h.

◆ NNPSMEFTd6Vars

const int NPSMEFTd6::NNPSMEFTd6Vars = 446
static

The number of the model parameters in NPSMEFTd6.

 

Definition at line 831 of file NPSMEFTd6.h.

◆ NNPSMEFTd6Vars_LFU_QFU

const int NPSMEFTd6::NNPSMEFTd6Vars_LFU_QFU = 250
static

The number of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities.

 

Definition at line 849 of file NPSMEFTd6.h.

◆ NPSMEFTd6M

Matching<NPSMEFTd6Matching,NPSMEFTd6> NPSMEFTd6::NPSMEFTd6M
mutableprotected

Definition at line 4411 of file NPSMEFTd6.h.

◆ NPSMEFTd6Vars

const std::string NPSMEFTd6::NPSMEFTd6Vars
static

A string array containing the labels of the model parameters in NPSMEFTd6 if the model flag FlagRotateCHWCHB=false.

Definition at line 837 of file NPSMEFTd6.h.

◆ NPSMEFTd6Vars_LFU_QFU

const std::string NPSMEFTd6::NPSMEFTd6Vars_LFU_QFU
static

A string array containing the labels of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities if the model flag FlagRotateCHWCHB=false.

Definition at line 856 of file NPSMEFTd6.h.

◆ NPSMEFTd6VarsRot

const std::string NPSMEFTd6::NPSMEFTd6VarsRot
static

A string array containing the labels of the model parameters in NPSMEFTd6 if the model flag FlagRotateCHWCHB=true.

Definition at line 843 of file NPSMEFTd6.h.

◆ NPSMEFTd6VarsRot_LFU_QFU

const std::string NPSMEFTd6::NPSMEFTd6VarsRot_LFU_QFU
static

A string array containing the labels of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities if the model flag FlagRotateCHWCHB=true.

Definition at line 863 of file NPSMEFTd6.h.

◆ sW2_tree

double NPSMEFTd6::sW2_tree
protected

The square of the tree level values for the sine of the weak angle.

Definition at line 4881 of file NPSMEFTd6.h.

◆ sW_tree

double NPSMEFTd6::sW_tree
protected

The tree level values for the sine of the weak angle.

Definition at line 4879 of file NPSMEFTd6.h.

◆ UevL

double NPSMEFTd6::UevL
protected

The tree level value of the \(W^-\bar{\ell}\nu\) couplings in the SM. (Neglecting PMNS effects.)

Definition at line 4892 of file NPSMEFTd6.h.

◆ v2

double NPSMEFTd6::v2
protected

The square of the EW vev.

Definition at line 4873 of file NPSMEFTd6.h.

◆ v2_over_LambdaNP2

double NPSMEFTd6::v2_over_LambdaNP2
protected

The ratio between the EW vev and the new physics scale, squared \(v^2/\Lambda^2\).

Definition at line 4874 of file NPSMEFTd6.h.

◆ VudL

double NPSMEFTd6::VudL
protected

The tree level value of the \(W^+\bar{u}d\) couplings in the SM. (Neglecting CKM effects.)

Definition at line 4893 of file NPSMEFTd6.h.

◆ w_WW

gsl_integration_cquad_workspace* NPSMEFTd6::w_WW
private

Gsl integral variable

Definition at line 5005 of file NPSMEFTd6.h.

◆ Yukb

double NPSMEFTd6::Yukb
protected

SM d-quark Yukawas.

Definition at line 4912 of file NPSMEFTd6.h.

◆ Yukc

double NPSMEFTd6::Yukc
protected

Definition at line 4911 of file NPSMEFTd6.h.

◆ Yukd

double NPSMEFTd6::Yukd
protected

Definition at line 4912 of file NPSMEFTd6.h.

◆ Yuke

double NPSMEFTd6::Yuke
protected

Definition at line 4910 of file NPSMEFTd6.h.

◆ Yukmu

double NPSMEFTd6::Yukmu
protected

Definition at line 4910 of file NPSMEFTd6.h.

◆ Yuks

double NPSMEFTd6::Yuks
protected

Definition at line 4912 of file NPSMEFTd6.h.

◆ Yukt

double NPSMEFTd6::Yukt
protected

SM u-quark Yukawas.

Definition at line 4911 of file NPSMEFTd6.h.

◆ Yuktau

double NPSMEFTd6::Yuktau
protected

SM lepton Yukawas.

Definition at line 4910 of file NPSMEFTd6.h.

◆ Yuku

double NPSMEFTd6::Yuku
protected

Definition at line 4911 of file NPSMEFTd6.h.


The documentation for this class was generated from the following files:
QCD::TAU
Definition: QCD.h:316
NPSMEFTd6::CHud_12i
double CHud_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4503
NPSMEFTd6::deltaMwd6
virtual double deltaMwd6() const
The relative NP corrections to the mass of the boson, .
Definition: NPSMEFTd6.cpp:2751
NPSMEFTd6::eggFHZZ
double eggFHZZ
Definition: NPSMEFTd6.h:4664
NPSMEFTd6::CuB_23r
double CuB_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4572
NPSMEFTd6::CHud_33r
double CHud_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4501
sigmattH
Definition: NPSMEFT6dtopquark.h:606
NPSMEFTd6::lambZ
double lambZ
Independent contribution to aTGC.
Definition: NPSMEFTd6.h:4799
NPSMEFTd6::deltaGammaTotalRatio1noError
virtual double deltaGammaTotalRatio1noError() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:10607
NPSMEFTd6::CpLedQ_11
double CpLedQ_11
Definition: NPSMEFTd6.h:4622
NPSMEFTd6::C2BS
double C2BS
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4417
NPSMEFTd6::delta_ZZ
double delta_ZZ
Combination of dimension 6 coefficients modifying the canonical field definition.
Definition: NPSMEFTd6.h:4895
gslpp::cos
complex cos(const complex &z)
Definition: gslpp_complex.cpp:429
NPSMEFTd6::Yuku
double Yuku
Definition: NPSMEFTd6.h:4911
NPSMEFTd6::eggFHtautau
double eggFHtautau
Definition: NPSMEFTd6.h:4664
NPSMEFTd6::g3_tree
double g3_tree
The tree level value of the gauge coupling contant (at the pole).
Definition: NPSMEFTd6.h:4885
NPSMEFTd6::CLQ1_3113
double CLQ1_3113
Definition: NPSMEFTd6.h:4585
NPSMEFTd6::CLu_2211
double CLu_2211
Definition: NPSMEFTd6.h:4609
QCD::NEUTRINO_3
Definition: QCD.h:315
NPSMEFTd6::CLQ3_3113
double CLQ3_3113
Definition: NPSMEFTd6.h:4590
NPSMEFTd6::GammaHmumuRatio
double GammaHmumuRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:12153
NPSMEFTd6::CHL1_23i
double CHL1_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4441
NPSMEFTd6::CLd_2211
double CLd_2211
Definition: NPSMEFTd6.h:4613
NPSMEFTd6::deltag1ZNP
virtual double deltag1ZNP() const
The new physics contribution to the anomalous triple gauge coupling .
Definition: NPSMEFTd6.cpp:13495
NPSMEFTd6::obliqueS
virtual double obliqueS() const
The oblique parameter . (Simplified implementation. Contribution only from .)
Definition: NPSMEFTd6.cpp:2603
NPSMEFTd6::dxseeWWdcosBin
virtual double dxseeWWdcosBin(const double sqrt_s, const double cos1, const double cos2) const
The integral of differential distribution for , with in a given bin of the polar angle.
Definition: NPSMEFTd6.cpp:13864
NPSMEFTd6::ettH_78_uG_33r
double ettH_78_uG_33r
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPSMEFTd6.h:4786
StandardModel::cW2
virtual double cW2(const double Mw_i) const
The square of the cosine of the weak mixing angle in the on-shell scheme, denoted as .
Definition: StandardModel.cpp:989
NPSMEFTd6::CHud_11r
double CHud_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4496
NPSMEFTd6::CiH
double CiH
Definition: NPSMEFTd6.h:4844
NPSMEFTd6::eWH_1314_HW
double eWH_1314_HW
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:4735
NPSMEFTd6::eVBF_1314_DeltaGF
double eVBF_1314_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4714
NPSMEFTd6::eHWWpar
double eHWWpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:4648
StandardModel::setParameter
virtual void setParameter(const std::string name, const double &value)
A method to set the value of a parameter of StandardModel.
Definition: StandardModel.cpp:231
NPSMEFTd6::deltaGammaHZeeRatio2
double deltaGammaHZeeRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11275
StandardModel::v
virtual double v() const
The Higgs vacuum expectation value.
Definition: StandardModel.cpp:917
NPSMEFTd6::GammaW
virtual double GammaW() const
The total width of the boson, .
Definition: NPSMEFTd6.cpp:2813
NPSMEFTd6::ettHbb
double ettHbb
Definition: NPSMEFTd6.h:4668
NPSMEFTd6::gZlL
double gZlL
Definition: NPSMEFTd6.h:4888
NPSMEFTd6::CHd_23r
double CHd_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4491
NPSMEFTd6::Yukmu
double Yukmu
Definition: NPSMEFTd6.h:4910
NPSMEFTd6::deltaGammaHZuuRatio2
double deltaGammaHZuuRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11774
NPSMEFTd6::CeH_11r
double CeH_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4508
NPSMEFTd6::aiT
double aiT
Definition: NPSMEFTd6.h:4916
NPSMEFTd6::CQe_2333
double CQe_2333
Definition: NPSMEFTd6.h:4620
NPSMEFTd6::cW2_tree
double cW2_tree
The square of the tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:4880
NPSMEFTd6::CHQ1_33
double CHQ1_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4465
NPSMEFTd6::deltaGammaHZmumuRatio2
double deltaGammaHZmumuRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11336
NPSMEFTd6::eHggpar
double eHggpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:4646
NPSMEFTd6::obliqueT
virtual double obliqueT() const
The oblique parameter . (Simplified implementation. Contribution only from .)
Definition: NPSMEFTd6.cpp:2608
QCD::BOTTOM
Definition: QCD.h:329
NPSMEFTd6::CLd_1132
double CLd_1132
Definition: NPSMEFTd6.h:4616
NPSMEFTd6::eZH_2_Hd_11
double eZH_2_Hd_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4743
NPSMEFTd6::deltaGammaHmumuRatio1
double deltaGammaHmumuRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:12169
NPSMEFTd6::CiHd_33
double CiHd_33
Definition: NPSMEFTd6.h:4832
NPSMEFTd6::deltaGammaHZZ4muRatio2
double deltaGammaHZZ4muRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11594
NPSMEFTd6::eZHbb
double eZHbb
Definition: NPSMEFTd6.h:4667
NPSMEFTd6::NNPSMEFTd6Vars
static const int NNPSMEFTd6Vars
The number of the model parameters in NPSMEFTd6.
Definition: NPSMEFTd6.h:831
NPSMEFTd6::gZlR
double gZlR
The tree level value of the couplings in the SM.
Definition: NPSMEFTd6.h:4888
NPSMEFTd6::Ceu_1111
double Ceu_1111
Definition: NPSMEFTd6.h:4596
NPSMEFTd6::BrHZZ4muRatio
virtual double BrHZZ4muRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10167
NPSMEFTd6::CuW_13r
double CuW_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4558
NPSMEFTd6::cgg_HB
virtual double cgg_HB() const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
Definition: NPSMEFTd6.cpp:15256
NPSMEFTd6::CeH_23r
double CeH_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4512
NPSMEFTd6::CLd_2223
double CLd_2223
Definition: NPSMEFTd6.h:4615
NPSMEFTd6::CLQ1_1331
double CLQ1_1331
Definition: NPSMEFTd6.h:4585
NPSMEFTd6::CLQ1_2211
double CLQ1_2211
Definition: NPSMEFTd6.h:4584
NPSMEFTd6::CuG_12i
double CuG_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4551
Particle::is
bool is(std::string name_i) const
Definition: Particle.cpp:23
NPSMEFTd6::deltaGammaHbbRatio2
double deltaGammaHbbRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:12379
NPSMEFTd6::ettH_1314_G
double ettH_1314_G
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPSMEFTd6.h:4790
StandardModel::computeSigmaWH
double computeSigmaWH(const double sqrt_s) const
The WH production cross section in the Standard Model.
Definition: StandardModel.h:2088
NPSMEFTd6::CLQ1_2232
double CLQ1_2232
Definition: NPSMEFTd6.h:4587
NPSMEFTd6::CiHB
double CiHB
Definition: NPSMEFTd6.h:4837
NPSMEFTd6::deltaGammaHZgaRatio1
double deltaGammaHZgaRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:12008
NPSMEFTd6::eWH_78_HQ3_11
double eWH_78_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:4725
StandardModel::gamma
double gamma
used as an input for FlagWolfenstein = FALSE
Definition: StandardModel.h:2531
NPSMEFTd6::CLQ3_1133
double CLQ3_1133
Definition: NPSMEFTd6.h:4590
NPSMEFTd6::eHggint
double eHggint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:4645
NPSMEFTd6::CLQ1_1123
double CLQ1_1123
Definition: NPSMEFTd6.h:4586
NPSMEFTd6::eZHmumu
double eZHmumu
Total relative theoretical error in .
Definition: NPSMEFTd6.h:4667
NPSMEFTd6::ettH_1314_DeltagHt
double ettH_1314_DeltagHt
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPSMEFTd6.h:4792
NPSMEFTd6::C2W
double C2W
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4416
NPSMEFTd6::eWH_2_Hbox
double eWH_2_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:4716
NPSMEFTd6::eZH_1314_HB
double eZH_1314_HB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4772
NPSMEFTd6::CLd_1111
double CLd_1111
Definition: NPSMEFTd6.h:4612
NPSMEFTd6::CidH_22r
double CidH_22r
Definition: NPSMEFTd6.h:4855
gslpp::matrix< double >
A class for constructing and defining operations on real matrices.
Definition: gslpp_matrix_double.h:48
NPSMEFTd6::CHd_11
double CHd_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4487
NPSMEFTd6::CLd_3332
double CLd_3332
Definition: NPSMEFTd6.h:4616
NPSMEFTd6::CHe_23i
double CHe_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4459
NPSMEFTd6::deltayc_HB
virtual double deltayc_HB() const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
Definition: NPSMEFTd6.cpp:15178
NPSMEFTd6::FlagHiggsSM
bool FlagHiggsSM
A boolean flag that is true if including dependence on small variations of the SM parameters (depende...
Definition: NPSMEFTd6.h:4989
NPSMEFTd6::CiLL_2112
double CiLL_2112
Definition: NPSMEFTd6.h:4871
NPSMEFTd6::CLe_2211
double CLe_2211
Definition: NPSMEFTd6.h:4606
NPSMEFTd6::muVH
virtual double muVH(const double sqrt_s) const
The ratio between the WH+ZH associated production cross-section in the current model and in the Stan...
Definition: NPSMEFTd6.cpp:8726
NPSMEFTd6::CHf_diag
double CHf_diag(const Particle f) const
The diagonal entry of the dimension-6 operator coefficient corresponding to particle f.
Definition: NPSMEFTd6.cpp:2450
NPSMEFTd6::CHud_33i
double CHud_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4507
NPSMEFTd6::CidH_33r
double CidH_33r
Definition: NPSMEFTd6.h:4856
NPSMEFTd6::CdH_22r
double CdH_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4535
NPSMEFTd6::CLedQ_22
double CLedQ_22
Definition: NPSMEFTd6.h:4622
NPSMEFTd6::CHud_13r
double CHud_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4498
NPSMEFTd6::BrHtautauRatio
virtual double BrHtautauRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10490
NPSMEFTd6::eHZgapar
double eHZgapar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:4652
NPSMEFTd6Matching::updateNPSMEFTd6Parameters
void updateNPSMEFTd6Parameters()
Updates to new FlavourWilsonCoefficient parameter sets.
Definition: NPSMEFTd6Matching.cpp:24
NPSMEFTd6::eWHWW
double eWHWW
Definition: NPSMEFTd6.h:4666
NPSMEFTd6::CHu_12i
double CHu_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4484
NPSMEFTd6::CiHQ1_22
double CiHQ1_22
Definition: NPSMEFTd6.h:4816
NPSMEFTd6::CHL3_12i
double CHL3_12i
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4448
NPSMEFTd6::eepZBFint
double eepZBFint
Intrinsic relative theoretical error in via ZBF. (Assumed to be constant in energy....
Definition: NPSMEFTd6.h:4643
StandardModel::computeBrHtotautau
double computeBrHtotautau() const
The Br in the Standard Model.
Definition: StandardModel.h:2264
NPSMEFTd6::CHu_13r
double CHu_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4480
NPSMEFTd6::CQe_3222
double CQe_3222
Definition: NPSMEFTd6.h:4621
NPSMEFTd6::BrHgagaRatio
virtual double BrHgagaRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10438
NPSMEFTd6::CHQ1_13i
double CHQ1_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4467
NPSMEFTd6::aleMz
double aleMz
The em constant at Mz.
Definition: NPSMEFTd6.h:4875
NPSMEFTd6::deltamtau
virtual double deltamtau() const
The relative correction to the mass of the lepton, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:2685
NPSMEFTd6::eZHint
double eZHint
Intrinsic relative theoretical error in ZH production. (Assumed to be constant in energy....
Definition: NPSMEFTd6.h:4633
NPSMEFTd6::eZH_2_HW
double eZH_2_HW
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4747
NPSMEFTd6::CHe_23r
double CHe_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4455
NPSMEFTd6::CLQ3_2211
double CLQ3_2211
Definition: NPSMEFTd6.h:4589
NPSMEFTd6::deltaGammaHZmumuRatio1
double deltaGammaHZmumuRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11301
NPSMEFTd6::deltaGammaHZZ4vRatio2
double deltaGammaHZZ4vRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11715
NPSMEFTd6::CHQ1_23i
double CHQ1_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4468
NPSMEFTd6::CuB_22r
double CuB_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4571
NPSMEFTd6::ettH_2_DeltagHt
double ettH_2_DeltagHt
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPSMEFTd6.h:4782
NPSMEFTd6::Ceu_2211
double Ceu_2211
Definition: NPSMEFTd6.h:4597
NPSMEFTd6::CLL_1122
double CLL_1122
Definition: NPSMEFTd6.h:4581
NPSMEFTd6::deltaGammaHWW4fRatio2
double deltaGammaHWW4fRatio2() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
Definition: NPSMEFTd6.cpp:11107
NPSMEFTd6::Ceu_1133
double Ceu_1133
Definition: NPSMEFTd6.h:4598
NPSMEFTd6::Ceu_3311
double Ceu_3311
Definition: NPSMEFTd6.h:4598
NPSMEFTd6::CuG_23i
double CuG_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4554
NPSMEFTd6::aiHQ
double aiHQ
Definition: NPSMEFTd6.h:4918
NPSMEFTd6::CdH_13i
double CdH_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4540
NPSMEFTd6::g1_tree
double g1_tree
The tree level value of the gauge coupling contant (at the pole).
Definition: NPSMEFTd6.h:4883
NPSMEFTd6::CQe_3211
double CQe_3211
Definition: NPSMEFTd6.h:4621
NPSMEFTd6::BrHbbRatio
virtual double BrHbbRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10542
NPSMEFTd6::CHQ3_22
double CHQ3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4472
NPSMEFTd6::FlagLoopHd6
bool FlagLoopHd6
A boolean flag that is true if including modifications in the SM loops in Higgs observables due to th...
Definition: NPSMEFTd6.h:4990
NPSMEFTd6::Yukt
double Yukt
SM u-quark Yukawas.
Definition: NPSMEFTd6.h:4911
NPSMEFTd6::eHgagapar
double eHgagapar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:4654
NPSMEFTd6::GammaHTotR
double GammaHTotR
NP contributions and Total to Higgs width ratio with SM.
Definition: NPSMEFTd6.h:4922
NPbase::NPbase
NPbase()
The default constructor.
Definition: NPbase.cpp:10
NPSMEFTd6::CHL1_13r
double CHL1_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4435
NPSMEFTd6::eHccint
double eHccint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:4659
NPSMEFTd6::eVHinv
double eVHinv
Total relative theoretical error in .
Definition: NPSMEFTd6.h:4669
NPSMEFTd6::eggFHgaga
double eggFHgaga
Definition: NPSMEFTd6.h:4664
NPSMEFTd6::CLQ3_1331
double CLQ3_1331
Definition: NPSMEFTd6.h:4590
NPSMEFTd6::deltayb_HB
virtual double deltayb_HB() const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
Definition: NPSMEFTd6.cpp:15156
NPSMEFTd6::aiA
double aiA
Definition: NPSMEFTd6.h:4917
NPSMEFTd6::CHL1_33
double CHL1_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4438
NPSMEFTd6::CHu_13i
double CHu_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4485
NPSMEFTd6::Mw
virtual double Mw() const
The mass of the boson, .
Definition: NPSMEFTd6.cpp:2743
NPSMEFTd6::CHd_13r
double CHd_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4489
gslpp::sin
complex sin(const complex &z)
Definition: gslpp_complex.cpp:420
NPSMEFTd6::Ced_2211
double Ced_2211
Definition: NPSMEFTd6.h:4601
NPSMEFTd6::eWHZZ
double eWHZZ
Definition: NPSMEFTd6.h:4666
NPSMEFTd6::deltaGammaHZZ4eRatio1
double deltaGammaHZZ4eRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11432
Matching::getObj
T & getObj()
Definition: Matching.h:14
NPSMEFTd6::CLd_3323
double CLd_3323
Definition: NPSMEFTd6.h:4615
NPbase::BR_Zf
virtual double BR_Zf(const Particle f) const
The Branching ratio of the boson into a given fermion pair, .
Definition: NPbase.cpp:262
NPSMEFTd6::eepWBFpar
double eepWBFpar
Parametric relative theoretical error in via WBF. (Assumed to be constant in energy....
Definition: NPSMEFTd6.h:4642
NPSMEFTd6::CLd_1122
double CLd_1122
Definition: NPSMEFTd6.h:4613
NPSMEFTd6::LambdaNP2
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:4805
NPSMEFTd6::deltamc
virtual double deltamc() const
The relative correction to the mass of the quark, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2674
NPSMEFTd6::CLedQ_11
double CLedQ_11
Definition: NPSMEFTd6.h:4622
NPSMEFTd6::FlagLoopH3d6Quad
bool FlagLoopH3d6Quad
A boolean flag that is true if including quadratic modifications in the SM loops in Higgs observables...
Definition: NPSMEFTd6.h:4991
NPSMEFTd6::deltaGammaHccRatio1
double deltaGammaHccRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:12274
NPSMEFTd6::deltaGammaHZgaRatio2
double deltaGammaHZgaRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:12067
NPSMEFTd6::Ced_3311
double Ced_3311
Definition: NPSMEFTd6.h:4602
NPSMEFTd6::CLu_2233
double CLu_2233
Definition: NPSMEFTd6.h:4611
NPSMEFTd6::dKappaga
double dKappaga
Independent contribution to aTGC.
Definition: NPSMEFTd6.h:4798
NPSMEFTd6::deltaGammaHWW4fRatio1
double deltaGammaHWW4fRatio1() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
Definition: NPSMEFTd6.cpp:11063
NPSMEFTd6::CuW_11i
double CuW_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4562
NPSMEFTd6::CLu_3311
double CLu_3311
Definition: NPSMEFTd6.h:4610
QCD::UP
Definition: QCD.h:324
NPSMEFTd6::CieH_11r
double CieH_11r
Definition: NPSMEFTd6.h:4846
NPSMEFTd6::eZH_1314_Hu_11
double eZH_1314_Hu_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4768
StandardModel::GF
double GF
The Fermi constant in .
Definition: StandardModel.h:2511
NPSMEFTd6::CLQ1_2223
double CLQ1_2223
Definition: NPSMEFTd6.h:4586
NPSMEFTd6::deltaGammaHZvvRatio1
double deltaGammaHZvvRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11620
NPSMEFTd6::eVBF_1314_Hbox
double eVBF_1314_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4702
NPSMEFTd6::CHud_diag
gslpp::complex CHud_diag(const Particle u) const
The diagonal entry of the dimension-6 operator coefficient corresponding to particle f.
Definition: NPSMEFTd6.cpp:2476
NPSMEFTd6::Ced_3332
double Ced_3332
Definition: NPSMEFTd6.h:4604
NPSMEFTd6::CHe_33
double CHe_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4456
NPSMEFTd6::FlagPartialQFU
bool FlagPartialQFU
A boolean flag that is true if assuming partial quark flavour universality between the 1st and 2nd fa...
Definition: NPSMEFTd6.h:4986
NPSMEFTd6::CiuW_33r
double CiuW_33r
Definition: NPSMEFTd6.h:4864
Model::addMissingModelParameter
void addMissingModelParameter(const std::string &missingParameterName)
Definition: Model.h:232
NPSMEFTd6::CHd_12r
double CHd_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4488
NPSMEFTd6::eVBFHgaga
double eVBFHgaga
Definition: NPSMEFTd6.h:4665
NPSMEFTd6::CHW
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4420
StandardModel::CheckParameters
virtual bool CheckParameters(const std::map< std::string, double > &DPars)
A method to check if all the mandatory parameters for StandardModel have been provided in model initi...
Definition: StandardModel.cpp:313
NPSMEFTd6::CDHW
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4425
NPSMEFTd6::muZH
virtual double muZH(const double sqrt_s) const
The ratio between the Z-Higgs associated production cross-section in the current model and in the St...
Definition: NPSMEFTd6.cpp:7033
NPSMEFTd6::CHud_22i
double CHud_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4505
StandardModel::alphaMz
double alphaMz() const
The electromagnetic coupling at the -mass scale, .
Definition: StandardModel.cpp:867
NPSMEFTd6::deltaG_hhhRatio
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:3134
NPSMEFTd6::CLQ3_1132
double CLQ3_1132
Definition: NPSMEFTd6.h:4592
NPSMEFTd6::NPSMEFTd6Vars_LFU_QFU
static const std::string NPSMEFTd6Vars_LFU_QFU[NNPSMEFTd6Vars_LFU_QFU]
A string array containing the labels of the model parameters in NPSMEFTd6 with lepton and quark flavo...
Definition: NPSMEFTd6.h:856
NPSMEFTd6::CQe_3233
double CQe_3233
Definition: NPSMEFTd6.h:4621
NPSMEFTd6::deltaG_hff
virtual gslpp::complex deltaG_hff(const Particle p) const
The new physics contribution to the coupling of the effective interaction .
Definition: NPSMEFTd6.cpp:3120
NPSMEFTd6::CiuB_33r
double CiuB_33r
Definition: NPSMEFTd6.h:4868
NPSMEFTd6::deltaGzd6
virtual double deltaGzd6() const
The relative NP corrections to the width of the boson, .
Definition: NPSMEFTd6.cpp:2830
NPSMEFTd6::BrHinv
double BrHinv
The branching ratio of invisible Higgs decays.
Definition: NPSMEFTd6.h:4794
QCD::CHARM
Definition: QCD.h:326
NPSMEFTd6::cZBox_HB
virtual double cZBox_HB() const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
Definition: NPSMEFTd6.cpp:15210
NPSMEFTd6::aiHB
double aiHB
Definition: NPSMEFTd6.h:4916
NPSMEFTd6::ai3G
double ai3G
Definition: NPSMEFTd6.h:4915
NPSMEFTd6::CQe_1122
double CQe_1122
Definition: NPSMEFTd6.h:4618
NPSMEFTd6::aipHQ
double aipHQ
Definition: NPSMEFTd6.h:4918
NPSMEFTd6::cW_tree
double cW_tree
The tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:4878
NPbase::deltaGamma_Z
virtual double deltaGamma_Z() const
The new physics contribution to the total decay width of the boson, .
Definition: NPbase.cpp:176
NPSMEFTd6::deltaGammaHZeeRatio1
double deltaGammaHZeeRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11240
NPSMEFTd6::CLQ1_1122
double CLQ1_1122
Definition: NPSMEFTd6.h:4584
StandardModel::computeBrHtobb
double computeBrHtobb() const
The Br in the Standard Model.
Definition: StandardModel.h:2299
NPSMEFTd6::eZHZZ
double eZHZZ
Definition: NPSMEFTd6.h:4667
NPSMEFTd6::eVBF_2_HWB
double eVBF_2_HWB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4682
NPSMEFTd6::deltaG1_hZA
virtual double deltaG1_hZA() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPSMEFTd6.cpp:2972
NPSMEFTd6::eZH_78_HQ3_11
double eZH_78_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4757
NPSMEFTd6::deltaGammaHZffRatio1
double deltaGammaHZffRatio1() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
Definition: NPSMEFTd6.cpp:11859
NPSMEFTd6::eVBF_1314_HD
double eVBF_1314_HD
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4707
NPSMEFTd6::CuB_13r
double CuB_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4570
NPSMEFTd6::eZH_78_HD
double eZH_78_HD
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4758
NPSMEFTd6::CHQ3_12i
double CHQ3_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4475
gslpp::complex
A class for defining operations on and functions of complex numbers.
Definition: gslpp_complex.h:35
Matching::setObj
void setObj(T &obji)
Definition: Matching.h:15
NPSMEFTd6::BrHexo
double BrHexo
The branching ratio of exotic (not invisible) Higgs decays.
Definition: NPSMEFTd6.h:4795
NPSMEFTd6::deltaa0
virtual double deltaa0() const
The relative correction to the electromagnetic constant at zero momentum, , with respect to ref....
Definition: NPSMEFTd6.cpp:2718
NPSMEFTd6::deltaGammaHZuuRatio1
double deltaGammaHZuuRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11741
StandardModel::mHl
double mHl
The Higgs mass in GeV.
Definition: StandardModel.h:2514
NPSMEFTd6::deltaGammaHZZ4muRatio1
double deltaGammaHZZ4muRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11557
NPSMEFTd6::eggFHWW
double eggFHWW
Definition: NPSMEFTd6.h:4664
QCD::NEUTRINO_2
Definition: QCD.h:313
NPSMEFTd6::dZH
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:4902
NPSMEFTd6::eWH_2_HWB
double eWH_2_HWB
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:4720
gslpp::log
complex log(const complex &z)
Definition: gslpp_complex.cpp:342
NPSMEFTd6::CLQ3_3332
double CLQ3_3332
Definition: NPSMEFTd6.h:4592
NPSMEFTd6::eZHgaga
double eZHgaga
Definition: NPSMEFTd6.h:4667
NPSMEFTd6::CiuW_11r
double CiuW_11r
Definition: NPSMEFTd6.h:4862
NPSMEFTd6::v2
double v2
The square of the EW vev.
Definition: NPSMEFTd6.h:4873
NPSMEFTd6::ettH_78_DeltagHt
double ettH_78_DeltagHt
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPSMEFTd6.h:4787
NPSMEFTd6::v2_over_LambdaNP2
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:4874
NPSMEFTd6::CLu_1111
double CLu_1111
Definition: NPSMEFTd6.h:4608
gslpp::matrix< gslpp::complex >
NPSMEFTd6::CuG_23r
double CuG_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4548
NPSMEFTd6::NPSMEFTd6VarsRot_LFU_QFU
static const std::string NPSMEFTd6VarsRot_LFU_QFU[NNPSMEFTd6Vars_LFU_QFU]
A string array containing the labels of the model parameters in NPSMEFTd6 with lepton and quark flavo...
Definition: NPSMEFTd6.h:863
NPSMEFTd6::CHL1_23r
double CHL1_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4437
NPSMEFTd6::CeH_12i
double CeH_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4515
NPSMEFTd6::CLQ3_3311
double CLQ3_3311
Definition: NPSMEFTd6.h:4590
NPSMEFTd6::CieH_22r
double CieH_22r
Definition: NPSMEFTd6.h:4847
NPSMEFTd6::CuG_12r
double CuG_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4545
NPSMEFTd6::gZdL
double gZdL
Definition: NPSMEFTd6.h:4890
NPSMEFTd6::CLd_2232
double CLd_2232
Definition: NPSMEFTd6.h:4616
NPSMEFTd6::eZHtautau
double eZHtautau
Definition: NPSMEFTd6.h:4667
NPSMEFTd6::deltaMh
virtual double deltaMh() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2641
NPSMEFTd6::ettH_1314_HG
double ettH_1314_HG
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPSMEFTd6.h:4789
NPSMEFTd6::CeH_33r
double CeH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4513
NPSMEFTd6::CiHW
double CiHW
Definition: NPSMEFTd6.h:4836
NPSMEFTd6::CeH_13i
double CeH_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4516
QCD::ELECTRON
Definition: QCD.h:312
NPSMEFTd6::eWH_1314_HD
double eWH_1314_HD
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:4734
cgagaHB
An observable class for the Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document....
Definition: NP_couplings.h:2996
Particle::getIsospin
double getIsospin() const
A get method to access the particle isospin.
Definition: Particle.h:115
NPSMEFTd6::CuH_22r
double CuH_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4523
NPSMEFTd6::eggFHZga
double eggFHZga
Definition: NPSMEFTd6.h:4664
NPSMEFTd6::FlagLeptonUniversal
const bool FlagLeptonUniversal
An internal boolean flag that is true if assuming lepton flavour universality.
Definition: NPSMEFTd6.h:4997
NPSMEFTd6::deltaGammaHWjjRatio2
double deltaGammaHWjjRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:10920
NPSMEFTd6::BrHmumuRatio
virtual double BrHmumuRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10464
NPSMEFTd6::deltaGammaHZddRatio2
double deltaGammaHZddRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11833
NPSMEFTd6::eZHpar
double eZHpar
Parametric relative theoretical error in ZH production. (Assumed to be constant in energy....
Definition: NPSMEFTd6.h:4634
NPSMEFTd6::CidH_11r
double CidH_11r
Definition: NPSMEFTd6.h:4854
gslpp::complex::abs2
double abs2() const
Definition: gslpp_complex.cpp:86
NPSMEFTd6::CHd_13i
double CHd_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4494
NPSMEFTd6::CuB_22i
double CuB_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4577
NPSMEFTd6::CuW_33r
double CuW_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4561
NPSMEFTd6::eVBF_78_DeltaGF
double eVBF_78_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4700
NPSMEFTd6::Ced_2223
double Ced_2223
Definition: NPSMEFTd6.h:4603
NPSMEFTd6::deltaG_hAA
virtual double deltaG_hAA() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPSMEFTd6.cpp:3062
NPSMEFTd6::deltamt
virtual double deltamt() const
The relative correction to the mass of the quark, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2652
NPSMEFTd6::CHWB
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4428
NPSMEFTd6::CHWHB_gaga
double CHWHB_gaga
The combination of dimension-6 operator coefficients entering in : .
Definition: NPSMEFTd6.h:4422
NPSMEFTd6::CiuB_11r
double CiuB_11r
Definition: NPSMEFTd6.h:4866
NPSMEFTd6::eZH_78_Hu_11
double eZH_78_Hu_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4755
NPSMEFTd6::CuH_13i
double CuH_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4528
NPSMEFTd6::CHL1_12i
double CHL1_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4439
StandardModel::SMM
Matching< StandardModelMatching, StandardModel > SMM
An object of type Matching.
Definition: StandardModel.h:2506
NPSMEFTd6::eggFHmumu
double eggFHmumu
Total relative theoretical error in .
Definition: NPSMEFTd6.h:4664
NPSMEFTd6::mueeZH
virtual double mueeZH(const double sqrt_s) const
The ratio between the associated production cross-section in the current model and in the Standard ...
Definition: NPSMEFTd6.cpp:7229
NPSMEFTd6::deltaGammaHZZRatio1
double deltaGammaHZZRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11133
NPSMEFTd6::eZH_1314_HW
double eZH_1314_HW
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4773
NPSMEFTd6::CuH_12r
double CuH_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4521
NPSMEFTd6::CQe_3311
double CQe_3311
Definition: NPSMEFTd6.h:4619
NPSMEFTd6::eZH_2_DHB
double eZH_2_DHB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4749
cZZHB
An observable class for the Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document....
Definition: NP_couplings.h:2920
NPSMEFTd6::deltaGammaHWW2l2vRatio2
double deltaGammaHWW2l2vRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:10864
NPSMEFTd6::CLd_3311
double CLd_3311
Definition: NPSMEFTd6.h:4614
NPSMEFTd6::ettH_78_G
double ettH_78_G
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPSMEFTd6.h:4785
NPSMEFTd6::eeMz2
double eeMz2
The em coupling squared (at Mz).
Definition: NPSMEFTd6.h:4877
NPSMEFTd6::CiHQ3_11
double CiHQ3_11
Definition: NPSMEFTd6.h:4818
NPSMEFTd6::eWH_1314_Hbox
double eWH_1314_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:4732
NPSMEFTd6::eggFHbb
double eggFHbb
Definition: NPSMEFTd6.h:4664
NPSMEFTd6::CHud_23i
double CHud_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4506
NPSMEFTd6::CpLedQ_22
double CpLedQ_22
Definition: NPSMEFTd6.h:4622
NPSMEFTd6::GammaHccRatio
double GammaHccRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:12258
NPSMEFTd6::eVBFHbb
double eVBFHbb
Definition: NPSMEFTd6.h:4665
NPSMEFTd6::Lambda_NP
double Lambda_NP
The new physics scale [GeV].
Definition: NPSMEFTd6.h:4623
NPSMEFTd6::CiuH_11r
double CiuH_11r
Definition: NPSMEFTd6.h:4850
NPSMEFTd6::Cee_2211
double Cee_2211
Definition: NPSMEFTd6.h:4594
NPSMEFTd6::CLQ1_1132
double CLQ1_1132
Definition: NPSMEFTd6.h:4587
NPSMEFTd6::eVBF_2_HW
double eVBF_2_HW
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4681
NPSMEFTd6::eZH_78_DeltaGF
double eZH_78_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4764
StandardModel::sW2
virtual double sW2(const double Mw_i) const
The square of the sine of the weak mixing angle in the on-shell scheme, denoted as .
Definition: StandardModel.cpp:1000
NPSMEFTd6::CuW_33i
double CuW_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4567
NPSMEFTd6::CiuB_22r
double CiuB_22r
Definition: NPSMEFTd6.h:4867
StandardModel::ale
double ale
The fine-structure constant .
Definition: StandardModel.h:2512
NPSMEFTd6::CHL3_13r
double CHL3_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4444
NPSMEFTd6::deltaGammaHWW2l2vRatio1
double deltaGammaHWW2l2vRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:10829
NPSMEFTd6::CHu_22
double CHu_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4481
NPSMEFTd6::AH_f
gslpp::complex AH_f(const double tau) const
Fermionic loop function entering in the calculation of the effective and couplings.
Definition: NPSMEFTd6.cpp:3271
QCD::mtpole
double mtpole
The pole mass of the top quark.
Definition: QCD.h:927
NPSMEFTd6::CHG
double CHG
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4419
NPSMEFTd6::eZH_78_HQ1_11
double eZH_78_HQ1_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4754
NPSMEFTd6::deltaGammaHggRatio2
double deltaGammaHggRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:10699
NPSMEFTd6::eVBF_2_DHW
double eVBF_2_DHW
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4685
NPSMEFTd6::eVBF_1314_HG
double eVBF_1314_HG
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4711
NPSMEFTd6::deltaGammaHWW4jRatio1
double deltaGammaHWW4jRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:10946
NPSMEFTd6::CiuH_33r
double CiuH_33r
Definition: NPSMEFTd6.h:4852
StandardModel::setFlag
virtual bool setFlag(const std::string name, const bool value)
A method to set a flag of StandardModel.
Definition: StandardModel.cpp:378
NPSMEFTd6::NPSMEFTd6VarsRot
static const std::string NPSMEFTd6VarsRot[NNPSMEFTd6Vars]
A string array containing the labels of the model parameters in NPSMEFTd6 if the model flag FlagRotat...
Definition: NPSMEFTd6.h:843
NPSMEFTd6::eZH_78_Hbox
double eZH_78_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4753
Model::ModelParamMap
std::map< std::string, std::reference_wrapper< const double > > ModelParamMap
Definition: Model.h:262
NPSMEFTd6::CLQ1_1221
double CLQ1_1221
Definition: NPSMEFTd6.h:4584
NPSMEFTd6::CHe_22
double CHe_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4454
NPSMEFTd6::CLL_1111
double CLL_1111
Definition: NPSMEFTd6.h:4580
NPSMEFTd6::deltaGammaHWffRatio1
double deltaGammaHWffRatio1() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
Definition: NPSMEFTd6.cpp:11006
NPSMEFTd6::eVBF_1314_DHB
double eVBF_1314_DHB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4712
NPSMEFTd6::CuG_11i
double CuG_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4550
NPSMEFTd6::VudL
double VudL
The tree level value of the couplings in the SM. (Neglecting CKM effects.)
Definition: NPSMEFTd6.h:4893
NPSMEFTd6::eVBF_2_HB
double eVBF_2_HB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4680
NPSMEFTd6::CuW_12i
double CuW_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4563
NPSMEFTd6::eVBF_78_HW
double eVBF_78_HW
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4695
NPSMEFTd6::gZuR
double gZuR
The tree level value of the couplings in the SM.
Definition: NPSMEFTd6.h:4889
NPSMEFTd6::g_triangle
gslpp::complex g_triangle(const double tau) const
Loop function entering in the calculation of the effective coupling.
Definition: NPSMEFTd6.cpp:3239
NPSMEFTd6::eVBF_1314_Hd_11
double eVBF_1314_Hd_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4705
NPSMEFTd6::GammaHZgaRatio
double GammaHZgaRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:11992
NPSMEFTd6::FlagQuarkUniversal
const bool FlagQuarkUniversal
An internal boolean flag that is true if assuming quark flavour universality.
Definition: NPSMEFTd6.h:5003
NPSMEFTd6::CHL3_33
double CHL3_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4447
NPSMEFTd6::Yukd
double Yukd
Definition: NPSMEFTd6.h:4912
NPSMEFTd6::CHd_33
double CHd_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4492
NPSMEFTd6::eVBF_2_HG
double eVBF_2_HG
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4683
NPSMEFTd6::ettH_2_uG_33r
double ettH_2_uG_33r
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPSMEFTd6.h:4781
NPSMEFTd6::eggFint
double eggFint
Intrinsic relative theoretical error in ggF production. (Assumed to be constant in energy....
Definition: NPSMEFTd6.h:4625
NPSMEFTd6::GammaHWWRatio
double GammaHWWRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10709
NPSMEFTd6::CuW_13i
double CuW_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4564
NPSMEFTd6::eHbbpar
double eHbbpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:4662
NPSMEFTd6::ai2G
double ai2G
Definition: NPSMEFTd6.h:4915
NPSMEFTd6::CHQ3_13i
double CHQ3_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4476
NPSMEFTd6::CiHL3_22
double CiHL3_22
Definition: NPSMEFTd6.h:4812
NPSMEFTd6::eHccpar
double eHccpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:4660
NPSMEFTd6::eZH_1314_DHB
double eZH_1314_DHB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4775
NPSMEFTd6::CHL1_13i
double CHL1_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4440
NPSMEFTd6::eeMz
double eeMz
The em coupling at Mz.
Definition: NPSMEFTd6.h:4876
NPSMEFTd6::CiHL1_33
double CiHL1_33
Definition: NPSMEFTd6.h:4810
NPSMEFTd6::deltaGammaHZZ4lRatio1
double deltaGammaHZZ4lRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11362
NPbase::trueSM
StandardModel trueSM
Definition: NPbase.h:2787
NPSMEFTd6::deltaGammaHWlvRatio2
double deltaGammaHWlvRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:10803
NPSMEFTd6::eWHint
double eWHint
Intrinsic relative theoretical error in WH production. (Assumed to be constant in energy....
Definition: NPSMEFTd6.h:4631
StandardModel::computeBrHtoZZ
double computeBrHtoZZ() const
The Br in the Standard Model.
Definition: StandardModel.h:2208
NPSMEFTd6::CHL3_11
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4442
NPSMEFTd6::eHtautauint
double eHtautauint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:4657
NPSMEFTd6::CuH_13r
double CuH_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4522
NPSMEFTd6::CLe_1133
double CLe_1133
Definition: NPSMEFTd6.h:4607
NPSMEFTd6::ettHint
double ettHint
Intrinsic relative theoretical error in ttH production. (Assumed to be constant in energy....
Definition: NPSMEFTd6.h:4627
NPSMEFTd6::CHF3_diag
double CHF3_diag(const Particle F) const
The diagonal entry of the dimension-6 operator coefficient corresponding to particle F.
Definition: NPSMEFTd6.cpp:2432
NPSMEFTd6::I_triangle_2
gslpp::complex I_triangle_2(const double tau, const double lambda) const
Loop function entering in the calculation of the effective coupling.
Definition: NPSMEFTd6.cpp:3262
NPSMEFTd6::eZH_1314_HWB
double eZH_1314_HWB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4774
NPSMEFTd6::cZZ_HB
virtual double cZZ_HB() const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
Definition: NPSMEFTd6.cpp:15222
NPSMEFTd6::eVBF_78_Hd_11
double eVBF_78_Hd_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4691
NPSMEFTd6::eWH_78_DeltaGF
double eWH_78_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (7...
Definition: NPSMEFTd6.h:4730
NPSMEFTd6::CuG_22i
double CuG_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4553
NPSMEFTd6::CiHe_33
double CiHe_33
Definition: NPSMEFTd6.h:4824
NPSMEFTd6::CHQ3_23i
double CHQ3_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4477
StandardModelMatching
A class for the matching in the Standard Model.
Definition: StandardModelMatching.h:26
NPSMEFTd6::GammaHtautauRatio
double GammaHtautauRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:12205
NPSMEFTd6::CHu_23i
double CHu_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4486
NPSMEFTd6::CiHL1_22
double CiHL1_22
Definition: NPSMEFTd6.h:4809
NPSMEFTd6::w_WW
gsl_integration_cquad_workspace * w_WW
Definition: NPSMEFTd6.h:5005
NPSMEFTd6::BrHWW2l2vRatio
virtual double BrHWW2l2vRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9936
NPSMEFTd6::CQe_2311
double CQe_2311
Definition: NPSMEFTd6.h:4620
gslpp::complex::conjugate
complex conjugate() const
Definition: gslpp_complex.cpp:288
NPSMEFTd6::eeeWBFint
double eeeWBFint
Intrinsic relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:4635
NPSMEFTd6::deltaaMZ
virtual double deltaaMZ() const
The relative correction to the electromagnetic constant at the Z pole, , with respect to ref....
Definition: NPSMEFTd6.cpp:2707
NPSMEFTd6::deltaGammaHgagaRatio1
double deltaGammaHgagaRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:12093
NPSMEFTd6::BrHZZ4lRatio
virtual double BrHZZ4lRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10092
Particle::getMass
const double & getMass() const
A get method to access the particle mass.
Definition: Particle.h:61
NPSMEFTd6::aiWW
double aiWW
Definition: NPSMEFTd6.h:4916
NPSMEFTd6::CdH_13r
double CdH_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4534
NPSMEFTd6::CHu_33
double CHu_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4483
NPSMEFTd6::aiuG
double aiuG
Definition: NPSMEFTd6.h:4919
NPSMEFTd6::CiuG_22r
double CiuG_22r
Definition: NPSMEFTd6.h:4859
NPSMEFTd6::eZH_2_DeltaGF
double eZH_2_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4751
NPSMEFTd6::CuG_33r
double CuG_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4549
NPSMEFTd6::CeH_22r
double CeH_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4511
NPSMEFTd6::CeH_13r
double CeH_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4510
NPSMEFTd6::CLQ1_3332
double CLQ1_3332
Definition: NPSMEFTd6.h:4587
NPSMEFTd6::CuH_22i
double CuH_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4529
NPSMEFTd6::deltaGmu
virtual double deltaGmu() const
The relative correction to the muon decay constant, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:2696
StandardModel::AlsMz
double AlsMz
The strong coupling constant at the Z-boson mass, .
Definition: StandardModel.h:2509
NPSMEFTd6::CQe_1111
double CQe_1111
Definition: NPSMEFTd6.h:4617
NPSMEFTd6::eZH_1314_Hd_11
double eZH_1314_Hd_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4769
NPSMEFTd6::ettHWW
double ettHWW
Definition: NPSMEFTd6.h:4668
NPSMEFTd6::eHmumupar
double eHmumupar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:4656
NPSMEFTd6::CHL3_22
double CHL3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4445
NPSMEFTd6::CiHu_22
double CiHu_22
Definition: NPSMEFTd6.h:4827
NPSMEFTd6::deltacZ_HB
virtual double deltacZ_HB() const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
Definition: NPSMEFTd6.cpp:15200
NPSMEFTd6::eepWBFint
double eepWBFint
Intrinsic relative theoretical error in via WBF. (Assumed to be constant in energy....
Definition: NPSMEFTd6.h:4641
NPSMEFTd6::CiHD
double CiHD
Definition: NPSMEFTd6.h:4843
NPSMEFTd6::deltaKgammaNP
virtual double deltaKgammaNP() const
The new physics contribution to the anomalous triple gauge coupling .
Definition: NPSMEFTd6.cpp:13512
NPSMEFTd6::CuB_33r
double CuB_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4573
NPSMEFTd6::ettHgaga
double ettHgaga
Definition: NPSMEFTd6.h:4668
NPSMEFTd6::eWH_1314_DeltaGF
double eWH_1314_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (1...
Definition: NPSMEFTd6.h:4738
NPSMEFTd6::eWHbb
double eWHbb
Definition: NPSMEFTd6.h:4666
NPSMEFTd6::eVBF_1314_HQ3_11
double eVBF_1314_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4706
NPSMEFTd6::CLu_1122
double CLu_1122
Definition: NPSMEFTd6.h:4609
NPSMEFTd6::FlagQuadraticTerms
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on.
Definition: NPSMEFTd6.h:4984
NPSMEFTd6::CLe_1111
double CLe_1111
Definition: NPSMEFTd6.h:4605
NPSMEFTd6::CuG_13r
double CuG_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4546
NPSMEFTd6::CiHu_11
double CiHu_11
Definition: NPSMEFTd6.h:4826
NPSMEFTd6::eWH_2_DeltaGF
double eWH_2_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (1...
Definition: NPSMEFTd6.h:4722
NPSMEFTd6::BrHZddRatio
virtual double BrHZddRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10282
QCD::TOP
Definition: QCD.h:328
NPSMEFTd6::CdH_33i
double CdH_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4543
NPSMEFTd6::AH_W
gslpp::complex AH_W(const double tau) const
W loop function entering in the calculation of the effective coupling.
Definition: NPSMEFTd6.cpp:3276
NPSMEFTd6::BrHZZRatio
virtual double BrHZZRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10062
NPSMEFTd6::eVBF_78_DHB
double eVBF_78_DHB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4698
NPSMEFTd6::eZH_1314_HD
double eZH_1314_HD
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4771
NPSMEFTd6::CdH_12r
double CdH_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4533
NPSMEFTd6::deltaGammaHZZ4fRatio1
double deltaGammaHZZ4fRatio1() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
Definition: NPSMEFTd6.cpp:11922
NPSMEFTd6::CLL_1221
double CLL_1221
Definition: NPSMEFTd6.h:4581
gslpp::pow
complex pow(const complex &z1, const complex &z2)
Definition: gslpp_complex.cpp:395
NPSMEFTd6::CLL_3311
double CLL_3311
Definition: NPSMEFTd6.h:4582
NPSMEFTd6::eZH_2_HD
double eZH_2_HD
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4745
NPSMEFTd6::eWHtautau
double eWHtautau
Definition: NPSMEFTd6.h:4666
NPSMEFTd6::cgaga_HB
virtual double cgaga_HB() const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
Definition: NPSMEFTd6.cpp:15246
NPSMEFTd6::CHe_13i
double CHe_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4458
NPSMEFTd6::eWH_2_HD
double eWH_2_HD
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:4718
NPSMEFTd6::eVBFHinv
double eVBFHinv
Definition: NPSMEFTd6.h:4669
NPSMEFTd6::aiHL
double aiHL
Definition: NPSMEFTd6.h:4918
NPSMEFTd6::eVBF_78_Hbox
double eVBF_78_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4688
NPSMEFTd6::Ced_1122
double Ced_1122
Definition: NPSMEFTd6.h:4601
Model::raiseMissingModelParameterCount
void raiseMissingModelParameterCount()
Definition: Model.h:242
NPSMEFTd6::mueeWBF
virtual double mueeWBF(const double sqrt_s) const
The ratio between the production cross-section in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:3694
gslpp::sqrt
complex sqrt(const complex &z)
Definition: gslpp_complex.cpp:385
NPSMEFTd6::delta_AZ
double delta_AZ
Combination of dimension 6 coefficients modifying the canonical field definition.
Definition: NPSMEFTd6.h:4897
NPSMEFTd6::cHSM
double cHSM
Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes.
Definition: NPSMEFTd6.h:4904
NPSMEFTd6::BrHWWRatio
virtual double BrHWWRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9904
NPSMEFTd6::eVBF_1314_DHW
double eVBF_1314_DHW
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4713
NPSMEFTd6::BrHtoinvRatio
virtual double BrHtoinvRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:12470
NPSMEFTd6::eVBF_1314_HB
double eVBF_1314_HB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4708
NPSMEFTd6::CHQ3_23r
double CHQ3_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4473
NPSMEFTd6::CQe_1133
double CQe_1133
Definition: NPSMEFTd6.h:4619
NPSMEFTd6::Ceu_1122
double Ceu_1122
Definition: NPSMEFTd6.h:4597
NPSMEFTd6::muggH
virtual double muggH(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section in the current model and in ...
Definition: NPSMEFTd6.cpp:3299
gslpp::complex::i
static const complex & i()
Definition: gslpp_complex.cpp:154
NPSMEFTd6::eWH_1314_DHW
double eWH_1314_DHW
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (1...
Definition: NPSMEFTd6.h:4737
NPSMEFTd6::CLQ1_3323
double CLQ1_3323
Definition: NPSMEFTd6.h:4586
NPSMEFTd6::eVBF_78_HD
double eVBF_78_HD
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4693
NPSMEFTd6::I_triangle_1
gslpp::complex I_triangle_1(const double tau, const double lambda) const
Loop function entering in the calculation of the effective coupling.
Definition: NPSMEFTd6.cpp:3251
NPSMEFTd6::CQe_2322
double CQe_2322
Definition: NPSMEFTd6.h:4620
StandardModel::computeBrHtoZga
double computeBrHtoZga() const
The Br in the Standard Model.
Definition: StandardModel.h:2230
NPSMEFTd6::CLd_1133
double CLd_1133
Definition: NPSMEFTd6.h:4614
NPSMEFTd6::CuB_12r
double CuB_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4569
StandardModel::lambda
double lambda
The CKM parameter in the Wolfenstein parameterization.
Definition: StandardModel.h:2524
Particle::getCharge
double getCharge() const
A get method to access the particle charge.
Definition: Particle.h:97
NPSMEFTd6::deltaG3_hWW
virtual double deltaG3_hWW() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPSMEFTd6.cpp:2944
NPSMEFTd6::deltaGL_f
double deltaGL_f(const Particle p) const
New physics contribution to the neutral-current left-handed coupling .
Definition: NPSMEFTd6.cpp:2852
NPSMEFTd6::deltaGammaTotalRatio1
virtual double deltaGammaTotalRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:10585
StandardModel::computeBrHtogaga
double computeBrHtogaga() const
The Br in the Standard Model.
Definition: StandardModel.h:2242
NPSMEFTd6::CiHe_22
double CiHe_22
Definition: NPSMEFTd6.h:4823
StandardModel::computeSigmaggH
double computeSigmaggH(const double sqrt_s) const
The ggH cross section in the Standard Model.
Definition: StandardModel.h:1883
NPSMEFTd6::CdH_22i
double CdH_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4541
NPSMEFTd6::CuH_33r
double CuH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4525
NPSMEFTd6::CHL3_23i
double CHL3_23i
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4450
NPSMEFTd6::CHu_12r
double CHu_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4479
NPSMEFTd6::eWHmumu
double eWHmumu
Total relative theoretical error in .
Definition: NPSMEFTd6.h:4666
NPSMEFTd6::eVBF_78_HG
double eVBF_78_HG
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4697
NPSMEFTd6::eVBF_1314_HWB
double eVBF_1314_HWB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4710
NPSMEFTd6::CHe_13r
double CHe_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4453
NPSMEFTd6::eZH_1314_Hbox
double eZH_1314_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4766
NPSMEFTd6::aipHL
double aipHL
Definition: NPSMEFTd6.h:4918
NPSMEFTd6::eVBFHtautau
double eVBFHtautau
Definition: NPSMEFTd6.h:4665
NPSMEFTd6::lambdaH_tree
double lambdaH_tree
The SM tree level value of the scalar quartic coupling in the potential.
Definition: NPSMEFTd6.h:4900
NPSMEFTd6::eVBFint
double eVBFint
Intrinsic relative theoretical error in VBF production. (Assumed to be constant in energy....
Definition: NPSMEFTd6.h:4629
NPSMEFTd6::eZH_1314_HQ3_11
double eZH_1314_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4770
NPSMEFTd6::UevL
double UevL
The tree level value of the couplings in the SM. (Neglecting PMNS effects.)
Definition: NPSMEFTd6.h:4892
NPSMEFTd6::cLH3d62
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:4908
NPSMEFTd6::ettHpar
double ettHpar
Parametric relative theoretical error in ttH production. (Assumed to be constant in energy....
Definition: NPSMEFTd6.h:4628
NPSMEFTd6::eVBF_2_HQ3_11
double eVBF_2_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4678
NPSMEFTd6::eZH_2_HQ1_11
double eZH_2_HQ1_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4741
NPSMEFTd6::CHQ1_11
double CHQ1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4460
NPSMEFTd6::CuH_11i
double CuH_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4526
NPSMEFTd6::Cee_1122
double Cee_1122
Definition: NPSMEFTd6.h:4594
NPSMEFTd6::eZH_1314_DeltaGF
double eZH_1314_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4777
StandardModel::computeSigmattH
double computeSigmattH(const double sqrt_s) const
The ttH production cross section in the Standard Model.
Definition: StandardModel.h:2157
NPSMEFTd6::CeH_33i
double CeH_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4519
NPSMEFTd6::CuW_11r
double CuW_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4556
NPSMEFTd6::eZHZga
double eZHZga
Definition: NPSMEFTd6.h:4667
NPSMEFTd6::deltaGammaHbbRatio1
double deltaGammaHbbRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:12339
NPSMEFTd6::CiDHW
double CiDHW
Definition: NPSMEFTd6.h:4839
NPSMEFTd6::AHZga_f
gslpp::complex AHZga_f(const double tau, const double lambda) const
Fermionic loop function entering in the calculation of the effective coupling.
Definition: NPSMEFTd6.cpp:3281
NPSMEFTd6::CuH_12i
double CuH_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4527
NPSMEFTd6::CiuG_11r
double CiuG_11r
Definition: NPSMEFTd6.h:4858
NPSMEFTd6::CdH_12i
double CdH_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4539
NPSMEFTd6::CQe_2211
double CQe_2211
Definition: NPSMEFTd6.h:4618
NPSMEFTd6::CLQ3_1111
double CLQ3_1111
Definition: NPSMEFTd6.h:4588
NPSMEFTd6::obliqueW
virtual double obliqueW() const
The oblique parameter . (Simplified implementation. Contribution only from .)
Definition: NPSMEFTd6.cpp:2618
NPSMEFTd6::deltaMz
virtual double deltaMz() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2630
NPSMEFTd6::deltaGwd6
virtual double deltaGwd6() const
The relative NP corrections to the width of the boson, .
Definition: NPSMEFTd6.cpp:2818
NPSMEFTd6::delta_AA
double delta_AA
Combination of dimension 6 coefficients modifying the canonical field definition.
Definition: NPSMEFTd6.h:4896
NPSMEFTd6::Cee_1111
double Cee_1111
Definition: NPSMEFTd6.h:4593
NPSMEFTd6::deltaGammaHgagaRatio2
double deltaGammaHgagaRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:12143
NPSMEFTd6::CHd_23i
double CHd_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4495
NPSMEFTd6::CLQ3_1122
double CLQ3_1122
Definition: NPSMEFTd6.h:4589
NPSMEFTd6::eZH_2_Hbox
double eZH_2_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4740
NPSMEFTd6::CiuG_33r
double CiuG_33r
Definition: NPSMEFTd6.h:4860
NPSMEFTd6::CHQ1_23r
double CHQ1_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4464
NPSMEFTd6::CLQ3_2223
double CLQ3_2223
Definition: NPSMEFTd6.h:4591
NPSMEFTd6::CHQ3_13r
double CHQ3_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4471
NPSMEFTd6::CHL1_22
double CHL1_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4436
NPSMEFTd6::CHL3_12r
double CHL3_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4443
NPSMEFTd6::deltamb
virtual double deltamb() const
The relative correction to the mass of the quark, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2663
NPSMEFTd6::CHe_12r
double CHe_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4452
NPSMEFTd6::eWHZga
double eWHZga
Definition: NPSMEFTd6.h:4666
NPSMEFTd6::CHud_13i
double CHud_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4504
NPSMEFTd6::CuH_33i
double CuH_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4531
NPSMEFTd6::eZH_78_HW
double eZH_78_HW
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4760
NPSMEFTd6::CiHQ3_22
double CiHQ3_22
Definition: NPSMEFTd6.h:4819
NPSMEFTd6::CieH_33r
double CieH_33r
Definition: NPSMEFTd6.h:4848
NPSMEFTd6::CG
double CG
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4413
NPSMEFTd6::CuB_12i
double CuB_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4575
NPSMEFTd6::cLHd6
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:4906
NPSMEFTd6::DeltaGF
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2598
NPSMEFTd6::CuB_13i
double CuB_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4576
NPSMEFTd6::CLQ3_3323
double CLQ3_3323
Definition: NPSMEFTd6.h:4591
NPSMEFTd6::eVBF_2_DHB
double eVBF_2_DHB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4684
StandardModel::GammaW
virtual double GammaW(const Particle fi, const Particle fj) const
A partial decay width of the boson decay into a SM fermion pair.
Definition: StandardModel.cpp:1140
cggHB
An observable class for the Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document....
Definition: NP_couplings.h:3034
NPSMEFTd6::BrHWW4fRatio
virtual double BrHWW4fRatio() const
The ratio of the Br , with any fermion, in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10037
NPSMEFTd6::delta_h
double delta_h
Combinations of dimension 6 coefficients modifying the canonical field definition.
Definition: NPSMEFTd6.h:4898
NPSMEFTd6::CHbox
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4431
NPSMEFTd6::CHF1_diag
double CHF1_diag(const Particle F) const
The diagonal entry of the dimension-6 operator coefficient corresponding to particle F.
Definition: NPSMEFTd6.cpp:2414
NPSMEFTd6::deltaG_hgg
virtual double deltaG_hgg() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPSMEFTd6.cpp:2907
NPSMEFTd6::deltaGL_Wff
virtual gslpp::complex deltaGL_Wff(const Particle pbar, const Particle p) const
New physics contribution to the charged current coupling .
Definition: NPSMEFTd6.cpp:2883
NPSMEFTd6::CuB_11r
double CuB_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4568
NPSMEFTd6::eepZBFpar
double eepZBFpar
Parametric relative theoretical error in via ZBF. (Assumed to be constant in energy....
Definition: NPSMEFTd6.h:4644
NPSMEFTd6::ettHZga
double ettHZga
Definition: NPSMEFTd6.h:4668
NPSMEFTd6::NNPSMEFTd6Vars_LFU_QFU
static const int NNPSMEFTd6Vars_LFU_QFU
The number of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities.
Definition: NPSMEFTd6.h:849
NPSMEFTd6::CeH_22i
double CeH_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4517
NPSMEFTd6::CHWHB_gagaorth
double CHWHB_gagaorth
The combination of dimension-6 operator coefficients .
Definition: NPSMEFTd6.h:4423
NPSMEFTd6::CiHd_22
double CiHd_22
Definition: NPSMEFTd6.h:4831
NPSMEFTd6::deltaGammaHZllRatio1
double deltaGammaHZllRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11181
NPSMEFTd6::eZHWW
double eZHWW
Definition: NPSMEFTd6.h:4667
NPSMEFTd6::dg1Z
double dg1Z
Independent contribution to aTGC.
Definition: NPSMEFTd6.h:4797
NPSMEFTd6::eZH_78_Hd_11
double eZH_78_Hd_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4756
NPSMEFTd6::eZH_78_HWB
double eZH_78_HWB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4761
NPSMEFTd6::CiuW_22r
double CiuW_22r
Definition: NPSMEFTd6.h:4863
NPSMEFTd6::eWHgaga
double eWHgaga
Definition: NPSMEFTd6.h:4666
NPSMEFTd6::eVBF_2_DeltaGF
double eVBF_2_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4686
NPSMEFTd6::CLL_1133
double CLL_1133
Definition: NPSMEFTd6.h:4582
NPSMEFTd6::eZH_1314_HQ1_11
double eZH_1314_HQ1_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4767
NPSMEFTd6::CHQ1_22
double CHQ1_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4463
NPSMEFTd6::eHgagaint
double eHgagaint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:4653
NPSMEFTd6::CuG_13i
double CuG_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4552
NPSMEFTd6::eHtautaupar
double eHtautaupar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:4658
NPSMEFTd6::CHB
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4421
NPSMEFTd6::NPSMEFTd6Vars
static const std::string NPSMEFTd6Vars[NNPSMEFTd6Vars]
A string array containing the labels of the model parameters in NPSMEFTd6 if the model flag FlagRotat...
Definition: NPSMEFTd6.h:837
NPSMEFTd6::deltaytau_HB
virtual double deltaytau_HB() const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
Definition: NPSMEFTd6.cpp:15167
NPSMEFTd6::eVBF_1314_Hu_11
double eVBF_1314_Hu_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4704
NPSMEFTd6::CiHd_11
double CiHd_11
Definition: NPSMEFTd6.h:4830
NPSMEFTd6::CLL_2211
double CLL_2211
Definition: NPSMEFTd6.h:4581
NPSMEFTd6::eZH_78_DHW
double eZH_78_DHW
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4763
NPSMEFTd6::eZH_78_DHB
double eZH_78_DHB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4762
NPSMEFTd6::gZuL
double gZuL
Definition: NPSMEFTd6.h:4889
NPSMEFTd6::deltaGammaHWWRatio2
double deltaGammaHWWRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:10745
NPSMEFTd6::sW2_tree
double sW2_tree
The square of the tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:4881
NPSMEFTd6::STXS_qqHqq_Rest
virtual double STXS_qqHqq_Rest(const double sqrt_s) const
The STXS bin .
Definition: NPSMEFTd6.cpp:14864
NPSMEFTd6::eVBF_2_Hbox
double eVBF_2_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4674
NPSMEFTd6::CH
double CH
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4432
NPSMEFTd6::Ced_3323
double Ced_3323
Definition: NPSMEFTd6.h:4603
NPSMEFTd6::CLd_1123
double CLd_1123
Definition: NPSMEFTd6.h:4615
NPSMEFTd6::ettHtautau
double ettHtautau
Definition: NPSMEFTd6.h:4668
NPSMEFTd6::CHQ3_12r
double CHQ3_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4470
NPSMEFTd6::Yuktau
double Yuktau
SM lepton Yukawas.
Definition: NPSMEFTd6.h:4910
NPSMEFTd6::lambdaZNP
virtual double lambdaZNP() const
The new physics contribution to the anomalous triple gauge coupling .
Definition: NPSMEFTd6.cpp:13526
NPSMEFTd6::muVBF
virtual double muVBF(const double sqrt_s) const
The ratio between the vector-boson fusion Higgs production cross-section in the current model and in...
Definition: NPSMEFTd6.cpp:3434
NPSMEFTd6::CHQ3_11
double CHQ3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4469
NPSMEFTd6::CLu_1133
double CLu_1133
Definition: NPSMEFTd6.h:4610
NPSMEFTd6::eVBFHmumu
double eVBFHmumu
Total relative theoretical error in .
Definition: NPSMEFTd6.h:4665
StandardModel::computeSigmaZH
double computeSigmaZH(const double sqrt_s) const
The ZH production cross section in the Standard Model.
Definition: StandardModel.h:2121
NPSMEFTd6::eVBF_2_Hd_11
double eVBF_2_Hd_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4677
NPSMEFTd6::CiHQ1_11
double CiHQ1_11
Definition: NPSMEFTd6.h:4815
NPSMEFTd6::Ced_1132
double Ced_1132
Definition: NPSMEFTd6.h:4604
NPSMEFTd6::CfH_diag
gslpp::complex CfH_diag(const Particle f) const
The diagonal entry of the dimension-6 operator coefficient corresponding to particle f.
Definition: NPSMEFTd6.cpp:2491
NPSMEFTd6::eeeWBFpar
double eeeWBFpar
Parametric relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:4636
NPSMEFTd6::deltaGamma_Wff
virtual double deltaGamma_Wff(const Particle fi, const Particle fj) const
The new physics contribution to the decay width of the boson into a given fermion pair,...
Definition: NPSMEFTd6.cpp:2766
NPSMEFTd6::CDHB
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4424
NPSMEFTd6::CdH_11r
double CdH_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4532
NPSMEFTd6::cZga_HB
virtual double cZga_HB() const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
Definition: NPSMEFTd6.cpp:15234
StandardModel::computeBrHtocc
double computeBrHtocc() const
The Br in the Standard Model.
Definition: StandardModel.h:2276
NPSMEFTd6::aiHW
double aiHW
Definition: NPSMEFTd6.h:4916
NPSMEFTd6::eHWWint
double eHWWint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:4647
NPSMEFTd6::eZH_2_DHW
double eZH_2_DHW
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4750
NPSMEFTd6::deltaGammaHZZ4vRatio1
double deltaGammaHZZ4vRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11678
NPSMEFTd6::CdH_11i
double CdH_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4538
NPSMEFTd6::CuB_33i
double CuB_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4579
NPSMEFTd6::eZH_78_HB
double eZH_78_HB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4759
NPSMEFTd6::eZH_1314_DHW
double eZH_1314_DHW
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4776
NPSMEFTd6::deltaGammaHZllRatio2
double deltaGammaHZllRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11214
NPSMEFTd6::FlagRotateCHWCHB
bool FlagRotateCHWCHB
A boolean flag that is true if we use as parameters CHWHB_gaga and CHWHB_gagaorth instead of CHW and ...
Definition: NPSMEFTd6.h:4985
NPSMEFTd6::CHd_22
double CHd_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4490
NPSMEFTd6::eZH_2_HB
double eZH_2_HB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4746
NPSMEFTd6::CLQ3_2112
double CLQ3_2112
Definition: NPSMEFTd6.h:4589
NPSMEFTd6::eWH_78_Hbox
double eWH_78_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:4724
NPSMEFTd6::deltaGammaHggRatio1
double deltaGammaHggRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:10664
StandardModel::Mw_tree
virtual double Mw_tree() const
The tree-level mass of the boson, .
Definition: StandardModel.cpp:925
NPSMEFTd6::BrHZuuRatio
virtual double BrHZuuRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10242
NPSMEFTd6::mueeZHPol
virtual double mueeZHPol(const double sqrt_s, const double Pol_em, const double Pol_ep) const
The ratio between the associated production cross-section in the current model and in the Standard ...
Definition: NPSMEFTd6.cpp:7586
NPSMEFTd6::BrHZZ4vRatio
virtual double BrHZZ4vRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10217
NPSMEFTd6::CuG_11r
double CuG_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4544
NPSMEFTd6::eWH_78_HD
double eWH_78_HD
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:4726
NPSMEFTd6::eWHpar
double eWHpar
Parametric relative theoretical error in WH production. (Assumed to be constant in energy....
Definition: NPSMEFTd6.h:4632
NPSMEFTd6::eHZZpar
double eHZZpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:4650
NPSMEFTd6::eVBF_78_HQ1_11
double eVBF_78_HQ1_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4689
StandardModel::computeBrHtomumu
double computeBrHtomumu() const
The Br in the Standard Model.
Definition: StandardModel.h:2253
NPSMEFTd6::eVBF_1314_HW
double eVBF_1314_HW
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4709
StandardModel::computeSigmaVBF
double computeSigmaVBF(const double sqrt_s) const
The VBF cross section in the Standard Model.
Definition: StandardModel.h:1989
NPSMEFTd6::deltaGammaHWWRatio1
double deltaGammaHWWRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:10725
NPSMEFTd6::eVBF_1314_HQ1_11
double eVBF_1314_HQ1_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4703
NPSMEFTd6::deltaGammaHZffRatio2
double deltaGammaHZffRatio2() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
Definition: NPSMEFTd6.cpp:11896
NPSMEFTd6::aiHd
double aiHd
Definition: NPSMEFTd6.h:4918
NPSMEFTd6::CuH_23r
double CuH_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4524
NPSMEFTd6::CDB
double CDB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4426
StandardModel::computeBrHtoWW
double computeBrHtoWW() const
The Br in the Standard Model.
Definition: StandardModel.h:2196
NPSMEFTd6::eeettHint
double eeettHint
Intrinsic relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:4639
NPSMEFTd6::eWH_78_HW
double eWH_78_HW
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:4727
NPSMEFTd6::CHud_12r
double CHud_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4497
NPSMEFTd6::Yukb
double Yukb
SM d-quark Yukawas.
Definition: NPSMEFTd6.h:4912
NPSMEFTd6::eggFpar
double eggFpar
Parametric relative theoretical error in ggF production. (Assumed to be constant in energy....
Definition: NPSMEFTd6.h:4626
NPSMEFTd6::CiHQ1_33
double CiHQ1_33
Definition: NPSMEFTd6.h:4817
NPSMEFTd6::aiHu
double aiHu
Definition: NPSMEFTd6.h:4918
NPSMEFTd6::deltaGammaHZZ2e2muRatio1
double deltaGammaHZZ2e2muRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11495
QCD::STRANGE
Definition: QCD.h:327
NPSMEFTd6::ettH_78_HG
double ettH_78_HG
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPSMEFTd6.h:4784
NPSMEFTd6::deltaaSMZ
virtual double deltaaSMZ() const
The relative correction to the strong coupling constant at the Z pole, , with respect to ref....
Definition: NPSMEFTd6.cpp:2729
NPSMEFTd6::CuW_23r
double CuW_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4560
NPSMEFTd6::deltaGammaHZvvRatio2
double deltaGammaHZvvRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11652
NPSMEFTd6::deltaGammaHZZ4fRatio2
double deltaGammaHZZ4fRatio2() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
Definition: NPSMEFTd6.cpp:11982
NPSMEFTd6::eVBF_2_Hu_11
double eVBF_2_Hu_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4676
NPSMEFTd6::eVBF_78_Hu_11
double eVBF_78_Hu_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4690
NPSMEFTd6::BrHZgaRatio
virtual double BrHZgaRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10375
NPSMEFTd6::eWH_2_DHW
double eWH_2_DHW
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (1...
Definition: NPSMEFTd6.h:4721
NPSMEFTd6::Cee_3311
double Cee_3311
Definition: NPSMEFTd6.h:4595
NPSMEFTd6::CiHu_33
double CiHu_33
Definition: NPSMEFTd6.h:4828
NPSMEFTd6::CLQ1_1111
double CLQ1_1111
Definition: NPSMEFTd6.h:4583
gslpp::complex::real
const double & real() const
Definition: gslpp_complex.cpp:53
NPSMEFTd6::Yuke
double Yuke
Definition: NPSMEFTd6.h:4910
NPSMEFTd6::CiHQ3_33
double CiHQ3_33
Definition: NPSMEFTd6.h:4820
NPSMEFTd6::CHud_23r
double CHud_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4500
NPSMEFTd6::deltaGammaHccRatio2
double deltaGammaHccRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:12314
NPSMEFTd6::ettHmumu
double ettHmumu
Total relative theoretical error in .
Definition: NPSMEFTd6.h:4668
NPSMEFTd6::Ced_1111
double Ced_1111
Definition: NPSMEFTd6.h:4600
StandardModel::leptons
Particle leptons[6]
An array of Particle objects for the leptons.
Definition: StandardModel.h:2496
NPSMEFTd6::g2_tree
double g2_tree
The tree level value of the gauge coupling contant (at the pole).
Definition: NPSMEFTd6.h:4884
NPSMEFTd6::aiB
double aiB
Definition: NPSMEFTd6.h:4916
NPSMEFTd6::deltaGammaHWlvRatio1
double deltaGammaHWlvRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:10773
NPSMEFTd6::deltaGammaHZZRatio2
double deltaGammaHZZRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11153
NPSMEFTd6::muttH
virtual double muttH(const double sqrt_s) const
The ratio between the t-tbar-Higgs associated production cross-section in the current model and in t...
Definition: NPSMEFTd6.cpp:8754
NPSMEFTd6::CiLL_1221
double CiLL_1221
Definition: NPSMEFTd6.h:4870
NPSMEFTd6::dGammaHTotR2
double dGammaHTotR2
Definition: NPSMEFTd6.h:4922
StandardModel::GammaZ
virtual double GammaZ(const Particle f) const
The partial decay width, .
Definition: StandardModel.cpp:1201
Particle::getIndex
int getIndex() const
Definition: Particle.h:160
NPSMEFTd6::CLQ3_1123
double CLQ3_1123
Definition: NPSMEFTd6.h:4591
NPSMEFTd6::BrHZgamumuRatio
virtual double BrHZgamumuRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10427
NPSMEFTd6::Cee_1133
double Cee_1133
Definition: NPSMEFTd6.h:4595
NPSMEFTd6::CuW_23i
double CuW_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4566
NPSMEFTd6::Ced_2232
double Ced_2232
Definition: NPSMEFTd6.h:4604
NPSMEFTd6::eVBFHZga
double eVBFHZga
Definition: NPSMEFTd6.h:4665
NPSMEFTd6::C2WS
double C2WS
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4418
NPSMEFTd6::CLL_1331
double CLL_1331
Definition: NPSMEFTd6.h:4582
NPSMEFTd6::GammaHZZRatio
double GammaHZZRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:11117
NPSMEFTd6::deltaGammaHtautauRatio2
double deltaGammaHtautauRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:12248
NPSMEFTd6::CHd_12i
double CHd_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4493
NPSMEFTd6::FlagUnivOfX
bool FlagUnivOfX
A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients and ...
Definition: NPSMEFTd6.h:4988
NPbase::PostUpdate
virtual bool PostUpdate()
The postupdate method for NPbase.
Definition: NPbase.cpp:23
StandardModel::computeBrHtogg
double computeBrHtogg() const
The Br in the Standard Model.
Definition: StandardModel.h:2185
NPSMEFTd6::CiHWB
double CiHWB
Definition: NPSMEFTd6.h:4840
NPSMEFTd6::Ced_1133
double Ced_1133
Definition: NPSMEFTd6.h:4602
Model::name
std::string name
The name of the model.
Definition: Model.h:267
NPSMEFTd6::aiH
double aiH
Definition: NPSMEFTd6.h:4916
NPSMEFTd6::aiHe
double aiHe
Definition: NPSMEFTd6.h:4918
StandardModel::Mz
double Mz
The mass of the boson in GeV.
Definition: StandardModel.h:2510
Model::setModelLinearized
void setModelLinearized(bool linearized=true)
Definition: Model.h:223
NPSMEFTd6::CLQ1_2112
double CLQ1_2112
Definition: NPSMEFTd6.h:4584
NPSMEFTd6::CiuH_22r
double CiuH_22r
Definition: NPSMEFTd6.h:4851
NPSMEFTd6::deltaGV_f
virtual double deltaGV_f(const Particle p) const
New physics contribution to the neutral-current vector coupling .
Definition: NPSMEFTd6.cpp:2842
NPSMEFTd6::deltaGammaHWffRatio2
double deltaGammaHWffRatio2() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
Definition: NPSMEFTd6.cpp:11037
NPSMEFTd6::ettH_2_HG
double ettH_2_HG
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPSMEFTd6.h:4779
NPSMEFTd6::CiHL1_11
double CiHL1_11
Definition: NPSMEFTd6.h:4808
NPSMEFTd6::eeeZHpar
double eeeZHpar
Parametric relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:4638
NPSMEFTd6::CLL_2112
double CLL_2112
Definition: NPSMEFTd6.h:4581
QCD::Nc
double Nc
The number of colours.
Definition: QCD.h:932
NPSMEFTd6::CiDHB
double CiDHB
Definition: NPSMEFTd6.h:4838
NPSMEFTd6::CiW
double CiW
Definition: NPSMEFTd6.h:4834
NPSMEFTd6::CHL1_11
double CHL1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4433
StandardModel::computeBrHtoZZinv
double computeBrHtoZZinv() const
The Br in the Standard Model.
Definition: StandardModel.h:2219
NPSMEFTd6::AHZga_W
gslpp::complex AHZga_W(const double tau, const double lambda) const
W loop function entering in the calculation of the effective coupling.
Definition: NPSMEFTd6.cpp:3286
NPSMEFTd6::BrHZZ4fRatio
virtual double BrHZZ4fRatio() const
The ratio of the Br , with any fermion, in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10350
NPSMEFTd6::CuB_11i
double CuB_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4574
NPSMEFTd6::dxseeWWdcos
virtual double dxseeWWdcos(const double sqrt_s, const double cos) const
The differential distribution for , with , as a function of the polar angle.
Definition: NPSMEFTd6.cpp:13565
NPSMEFTd6::eVBFpar
double eVBFpar
Parametric relative theoretical error in VBF production. (Assumed to be constant in energy....
Definition: NPSMEFTd6.h:4630
NPSMEFTd6::CeH_11i
double CeH_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4514
NPSMEFTd6::CuG_33i
double CuG_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4555
NPSMEFTd6::eeettHpar
double eeettHpar
Parametric relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:4640
lambdaZ
An observable class for the anomalous triple gauge coupling .
Definition: aTGC.h:99
NPSMEFTd6::f_triangle
gslpp::complex f_triangle(const double tau) const
Loop function entering in the calculation of the effective and couplings.
Definition: NPSMEFTd6.cpp:3227
NPSMEFTd6::CLQ3_1221
double CLQ3_1221
Definition: NPSMEFTd6.h:4589
NPSMEFTd6::CdH_23i
double CdH_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4542
StandardModel::Mw
virtual double Mw() const
The SM prediction for the -boson mass in the on-shell scheme, .
Definition: StandardModel.cpp:944
NPSMEFTd6::CDW
double CDW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4427
NPSMEFTd6::eZH_2_HWB
double eZH_2_HWB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4748
NPSMEFTd6::eWH_2_HQ3_11
double eWH_2_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:4717
NPSMEFTd6::eVBF_2_HQ1_11
double eVBF_2_HQ1_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4675
convertToGslFunction
gsl_function convertToGslFunction(const F &f)
Definition: gslpp_function_adapter.h:24
NPSMEFTd6::deltaGR_f
double deltaGR_f(const Particle p) const
New physics contribution to the neutral-current right-handed coupling .
Definition: NPSMEFTd6.cpp:2867
NPSMEFTd6::Ced_1123
double Ced_1123
Definition: NPSMEFTd6.h:4603
NPSMEFTd6::Ceu_2233
double Ceu_2233
Definition: NPSMEFTd6.h:4599
NPSMEFTd6::deltaGammaHWjjRatio1
double deltaGammaHWjjRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:10890
NPSMEFTd6::CeH_23i
double CeH_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4518
NPSMEFTd6::deltaGammaHZZ2e2muRatio2
double deltaGammaHZZ2e2muRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11532
NPSMEFTd6::CuG_22r
double CuG_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4547
NPSMEFTd6::muWH
virtual double muWH(const double sqrt_s) const
The ratio between the W-Higgs associated production cross-section in the current model and in the St...
Definition: NPSMEFTd6.cpp:6864
NPSMEFTd6::deltaGammaHmumuRatio2
double deltaGammaHmumuRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:12195
NPSMEFTd6::CHu_23r
double CHu_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4482
NPSMEFTd6::eVBF_78_HQ3_11
double eVBF_78_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4692
NPSMEFTd6::deltayt_HB
virtual double deltayt_HB() const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
Definition: NPSMEFTd6.cpp:15145
NPSMEFTd6::CiHL3_11
double CiHL3_11
Definition: NPSMEFTd6.h:4811
NPSMEFTd6::CLL_3113
double CLL_3113
Definition: NPSMEFTd6.h:4582
NPSMEFTd6::ettH_2_G
double ettH_2_G
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPSMEFTd6.h:4780
NPSMEFTd6::CeH_12r
double CeH_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4509
NPSMEFTd6::Yuks
double Yuks
Definition: NPSMEFTd6.h:4912
NPSMEFTd6::gZdR
double gZdR
The tree level value of the couplings in the SM.
Definition: NPSMEFTd6.h:4890
NPSMEFTd6::CLQ1_3311
double CLQ1_3311
Definition: NPSMEFTd6.h:4585
NPSMEFTd6::eeeZHint
double eeeZHint
Intrinsic relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:4637
NPSMEFTd6::CHe_12i
double CHe_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4457
NPSMEFTd6::C2B
double C2B
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4415
NPSMEFTd6::deltaGammaHtautauRatio1
double deltaGammaHtautauRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:12221
NPSMEFTd6::eWH_78_HWB
double eWH_78_HWB
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:4728
NPSMEFTd6::CHD
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4429
NPSMEFTd6::CLe_3311
double CLe_3311
Definition: NPSMEFTd6.h:4607
NPSMEFTd6::eHbbint
double eHbbint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:4661
NPSMEFTd6::eVBF_2_HD
double eVBF_2_HD
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4679
NPSMEFTd6::CuB_23i
double CuB_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4578
NPSMEFTd6::CHQ3_33
double CHQ3_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4474
NPSMEFTd6::eZH_2_HQ3_11
double eZH_2_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4744
NPSMEFTd6::deltaGammaHWW4jRatio2
double deltaGammaHWW4jRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:10980
NPSMEFTd6::deltaGammaHZddRatio1
double deltaGammaHZddRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11800
NPSMEFTd6::sW_tree
double sW_tree
The tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:4879
NPSMEFTd6::eVBFHZZ
double eVBFHZZ
Definition: NPSMEFTd6.h:4665
NPSMEFTd6::deltaGammaTotalRatio2
virtual double deltaGammaTotalRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:10629
NPSMEFTd6::CdH_33r
double CdH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4537
NPSMEFTd6::eHZgaint
double eHZgaint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:4651
NPSMEFTd6::eHZZint
double eHZZint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:4649
StandardModel::Gamma_Z
virtual double Gamma_Z() const
The total decay width of the boson, .
Definition: StandardModel.cpp:1318
NPSMEFTd6::CHQ1_12i
double CHQ1_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4466
NPSMEFTd6::deltaGamma_W
virtual double deltaGamma_W() const
The new physics contribution to the total decay width of the boson, .
Definition: NPSMEFTd6.cpp:2800
NPSMEFTd6::eWH_2_HW
double eWH_2_HW
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:4719
NPSMEFTd6::NPSMEFTd6M
Matching< NPSMEFTd6Matching, NPSMEFTd6 > NPSMEFTd6M
Definition: NPSMEFTd6.h:4411
NPSMEFTd6::eZH_2_Hu_11
double eZH_2_Hu_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4742
QCD::DOWN
Definition: QCD.h:325
cZgaHB
An observable class for the Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document....
Definition: NP_couplings.h:2958
NPSMEFTd6::eVBF_78_DHW
double eVBF_78_DHW
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4699
NPSMEFTd6::CHud_22r
double CHud_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4499
NPSMEFTd6::CuW_22r
double CuW_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4559
NPSMEFTd6::eWH_1314_HWB
double eWH_1314_HWB
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:4736
NPSMEFTd6::eVBFHWW
double eVBFHWW
Definition: NPSMEFTd6.h:4665
NPSMEFTd6::deltaGammaHZZ4eRatio2
double deltaGammaHZZ4eRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11469
NPSMEFTd6::CiHbox
double CiHbox
Definition: NPSMEFTd6.h:4842
NPSMEFTd6::CHQ1_12r
double CHQ1_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4461
NPSMEFTd6::ettH_1314_uG_33r
double ettH_1314_uG_33r
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPSMEFTd6.h:4791
NPSMEFTd6::eWH_78_DHW
double eWH_78_DHW
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (7...
Definition: NPSMEFTd6.h:4729
NPSMEFTd6::CT
double CT
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4430
NPSMEFTd6::CuW_12r
double CuW_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4557
NPSMEFTd6::dGammaHTotR1
double dGammaHTotR1
Definition: NPSMEFTd6.h:4922
NPSMEFTd6::CuW_22i
double CuW_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4565
NPSMEFTd6::eVBF_78_HB
double eVBF_78_HB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4694
NPSMEFTd6::GammaHggRatio
double GammaHggRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10648
NPSMEFTd6::CHQ1_13r
double CHQ1_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4462
NPSMEFTd6::CiHL3_33
double CiHL3_33
Definition: NPSMEFTd6.h:4813
NPSMEFTd6::CLQ3_2232
double CLQ3_2232
Definition: NPSMEFTd6.h:4592
NPSMEFTd6::CHe_11
double CHe_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4451
NPSMEFTd6::obliqueY
virtual double obliqueY() const
The oblique parameter . (Simplified implementation. Contribution only from .)
Definition: NPSMEFTd6.cpp:2623
NPSMEFTd6::GammaHbbRatio
double GammaHbbRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:12324
NPSMEFTd6::eHmumuint
double eHmumuint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:4655
NPSMEFTd6::eHwidth
double eHwidth
Total relative theoretical error in the Higgs width.
Definition: NPSMEFTd6.h:4671
NPSMEFTd6::deltaGammaHZZ4lRatio2
double deltaGammaHZZ4lRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11406
QCD::NEUTRINO_1
Definition: QCD.h:311
NPSMEFTd6::ettHZZ
double ettHZZ
Definition: NPSMEFTd6.h:4668
QCD::quarks
Particle quarks[6]
The vector of all SM quarks.
Definition: QCD.h:934
NPSMEFTd6::CHu_11
double CHu_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4478
NPSMEFTd6::CLQ1_1133
double CLQ1_1133
Definition: NPSMEFTd6.h:4585
NPSMEFTd6::CHud_11i
double CHud_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4502
NPSMEFTd6::CW
double CW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4414
NPSMEFTd6::aiu
double aiu
Definition: NPSMEFTd6.h:4919
NPSMEFTd6::eVBF_78_HWB
double eVBF_78_HWB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4696
NPSMEFTd6::CuH_11r
double CuH_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4520
NPSMEFTd6::gZvL
double gZvL
The tree level value of the couplings in the SM.
Definition: NPSMEFTd6.h:4887
QCD::MU
Definition: QCD.h:314
NPSMEFTd6::CHL3_23r
double CHL3_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4446
NPSMEFTd6::CuH_23i
double CuH_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4530
NPSMEFTd6::CiHe_11
double CiHe_11
Definition: NPSMEFTd6.h:4822
NPbase::deltaGamma_Zf
virtual double deltaGamma_Zf(const Particle f) const
The new physics contribution to the decay width of the boson into a given fermion pair,...
Definition: NPbase.cpp:135
NPSMEFTd6::aiG
double aiG
Definition: NPSMEFTd6.h:4915
NPSMEFTd6::Br_H_inv
virtual double Br_H_inv() const
The branching ratio of the of the Higgs into invisible particles.
Definition: NPSMEFTd6.cpp:12396
NPSMEFTd6::CdH_23r
double CdH_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4536
NPSMEFTd6::Yukc
double Yukc
Definition: NPSMEFTd6.h:4911
NPSMEFTd6::GammaHgagaRatio
double GammaHgagaRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:12077
NPSMEFTd6::CHL3_13i
double CHL3_13i
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4449
NPSMEFTd6::CLe_1122
double CLe_1122
Definition: NPSMEFTd6.h:4606
NPSMEFTd6::CHL1_12r
double CHL1_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4434
NPSMEFTd6::FlagFlavU3OfX
bool FlagFlavU3OfX
A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients.
Definition: NPSMEFTd6.h:4987
NPSMEFTd6::eWH_1314_HQ3_11
double eWH_1314_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:4733